The below are the simplest possible descriptions of various symbols, just to help you keep reading if you do not remember/know what they stand for. Don't cite them on a math test and then blame this book for your grade.

Watch it. There are so many ad hoc usages of symbols, some will have been overlooked here. Always use common sense first in guessing what a symbol means in a given context.

The quoted values of physical constants are usually taken from NIST CODATA in 2012 or later. The final digit of the listed value is normally doubtful. (It corresponds to the first nonzero digit of the standard deviation). Numbers ending in triple dots are exact and could be written down to more digits than listed if needed.

- A dot might indicate
- A dot product between vectors, if in between them.
- A time derivative of a quantity, if on top of it.

- Multiplication symbol. May indicate:
- An emphatic multiplication.
- Multiplication continued on the next line or from the previous line.
- A vectorial product between vectors. In index notation,
the
- th component ofequals

whereis the index following in the sequence 123123..., and the one preceding it (or second following). Alternatively, evaluate the determinant

- Might be used to indicate a factorial. Example:
5!
1 2 3 4 5 120. The function that generalizes

to noninteger values of is called the gamma function; . The gamma function generalization is due to, who else, Euler. (However, the fact thatinstead of is due to the idiocy of Legendre.) In Legendre-resistant notation,

Straightforward integration shows that 0! is 1 as it should, and integration by parts shows that, which ensures that the integral also produces the correct value offor any higher integer value of than 0. The integral, however, exists for any real value of above 1 , not just integers. The values of the integral are always positive, tending to positive infinity for both, (because the integral then blows up at small values of) , and for, (because the integral then blows up at medium-large values of) . In particular, Stirling’s formula says that for large positive, can be approximated as

where the value indicated by the dots becomes negligibly small for large. The functioncan be extended further to any complex value of , except the negative integer values of, whereis infinite, but is then no longer positive. Euler’s integral can be done for by making the change of variables , producing the integral, or, which equalsand the integral under the square root can be done analytically using polar coordinates. The result is that

To get, multiply by, since. A double exclamation mark may mean every second item is skipped, e.g. 5!!

1 3 5. In general, /. Of course, 5!! should logically mean (5!)!. Logic would indicate that 53 1 should be indicated by something like 5!’. But what is logic in physics? - May indicate:
- The magnitude or absolute value of the number or vector, if enclosed between a pair of them.
- The determinant of a matrix, if enclosed between a pair of them.
- The norm of the function, if enclosed between two pairs of them.
- The end of a bra or start of a ket.
- A visual separator in inner products.

- A
ket

is used to indicate some state. For example,indicates an angular momentum state with azimuthal quantum number and magnetic quantum number . Similarly,is the spin-down state of a particle with spin . Other common ones arefor the position eigenfunction , i.e., for the 1s or hydrogen state, for the 2 p orstate, etcetera. In short, whatever can indicate some state can be pushed into a ket. - A
bra

is like a ket, but appears in the left side of inner products, instead of the right one. - Indicates the
spin up

state. Mathematically, equals the functionwhich is by definition equal to 1 at and equal to 0 at . A spatial wave function multiplied byis a particle in that spatial state with its spin up. For multiple particles, the spins are listed with particle 1 first. - Indicates the
spin down

state. Mathematically, equals the functionwhich is by definition equal to 0 at and equal to 1 at . A spatial wave function multiplied byis a particle in that spatial state with its spin down. For multiple particles, the spins are listed with particle 1 first. - Summation symbol. Example: if in three
dimensional space a vector
has components 2, 1, 4, then stands for 7. One important thing to remember: the symbol used for the summation index does not make a difference:

is exactly the same as . So freely rename the index, but always make sure that the new name is not already used for something else in the part that it appears in. If you use the same name for two different things, it becomes a mess.Related to that,

is not something that depends on an index . It is just a combined simple number. Like 7 in the example above. It is commonly said that the summation indexsums away.

- (Not to be confused with
further down.) Multiplication symbol. Example: if in three dimensional space a vector has components 2, 1, 4, then stands for 6. One important thing to remember: the symbol used for the multiplications index does not make a difference:

is exactly the same as . So freely rename the index, but always make sure that the new name is not already used for something else in the part that it appears in. If you use the same name for two different things, it becomes a mess.Related to that,

is not something that depends on an index . It is just a combined simple number. Like 6 in the example above. It is commonly said that the multiplication indexfactors away.

(By who?) - Integration symbol, the continuous version of
the summation symbol. For example,

is the summation ofover all infinitesimally small fragments that make up the entire - range. For example,equals 3 2 6; the average value of between 0 and 2 is 3, and the sum of all the infinitesimally small segments gives the total length 2 of the range in from 0 to 2. One important thing to remember: the symbol used for the integration variable does not make a difference:

is exactly the same as . So freely rename the integration variable, but always make sure that the new name is not already used for something else in the part it appears in. If you use the same name for two different things, it becomes a mess.Related to that

is not something that depends on a variable . It is just a combined number. Like 6 in the example above. It is commonly said that the integration variableintegrates away.

- May indicate:
- An approaching process.
indicates for practical purposes the value of the expression following the when is extremely small. Similarly, indicates the value of the following expression when is extremely large. - The fact that the left side leads to, or implies, the right-hand side.

- An approaching process.
- Vector symbol. An arrow above a
letter indicates it is a vector. A vector is a quantity that
requires more than one number to be characterized. Typical vectors
in physics include position
, velocity, linear momentum, acceleration, force, angular momentum, etcetera. - A hat over a letter in this book indicates that it is the operator, turning functions into other functions.
- May indicate:
- A derivative of a function. Examples:
0, 1, , , . - A small or modified quantity.
- A quantity per unit length.

- A derivative of a function. Examples:
- The spatial differentiation operator
nabla. In Cartesian coordinates:

Nabla can be applied to a scalar function

in which case it gives a vector of partial derivatives called the gradient of the function:

Nabla can be applied to a vector in a dot product multiplication, in which case it gives a scalar function called the divergence of the vector:

or in index notation

Nabla can also be applied to a vector in a vectorial product multiplication, in which case it gives a vector function called the curl or rot of the vector. In index notation, the

- th component of this vector is

whereis the index following in the sequence 123123..., and the one preceding it (or the second following it). The operator

is called the Laplacian. In Cartesian coordinates:

Sometimes the Laplacian is indicated as. In relativistic index notation it is equal to, with maybe a minus sign depending on who you talk with.In non Cartesian coordinates, don’t guess; look these operators up in a table book, [41, pp. 124-126]: . For example, in spherical coordinates,

That allows the gradient of a scalar function

, i.e., to be found immediately. But if you applyon a vector, you have to be very careful because you also need to differentiate , , and. In particular, the correct divergence of a vectoris

The curlof the vector is

Finally the Laplacian is:

See alsospherical coordinates.

Cylindrical coordinates are usually indicated as

, and . Hereis the Cartesian coordinate, while is the distance from the - axis andthe angle around the axis. In two dimensions, i.e. without the terms, they are usually called polar coordinates. In cylindrical coordinates:

- The
D'Alembertian is defined as

whereis a constant called the wave speed. In relativistic index notation, is equal to . - A superscript star normally indicates a complex
conjugate. In the complex conjugate of a number, every
is changed into a . - Less than.
- Less than or equal.
- May indicate:
- An inner product.
- An expectation value.

- Greater than.
- Greater than or equal.
- May indicate:
- A grouping of terms in a formula.
- A commutator. For example,
.

- Equals sign. The quantity to the left is the same as the one to the right.
- Emphatic equals sign. Typically means “by
definition equal” or
everywhere equal.

- Indicates approximately equal. Read it as “is approximately equal to.”
- Indicates approximately equal. Often used when the
approximation applies only when something is small or large. Read
it as
is approximately equal to

or as “is asymptotically equal to.” - Proportional to. The two sides are equal except for some unknown constant factor.
- (alpha) May indicate:
- The fine structure constant,
/, equal to 7.297 352 570 10, or about 1/137, in value. - A Dirac equation matrix.
- A nuclear decay mode in which a helium-4 nucleus is emitted.
- Internal conversion rate as fraction of the gamma decay rate.
- Some constant.
- Some angle.
- An eigenfunction of a generic operator
. - A summation index.
- Component index of a vector.

- The fine structure constant,
- (beta) May indicate:
- A nuclear decay mode in which an electron
() or positron() is emitted. Sometimesis taken to also include electron capture. - A nuclear vibrational mode that maintains the axial symmetry of the nucleus.
- Some constant.
- Some angle.
- An eigenfunction of a generic operator
. - A summation index.

- A nuclear decay mode in which an electron
- (Gamma) May indicate:
- The Gamma function. Look under
!

for details. - The
width

or uncertainty in energy of an approximate energy eigenstate. - Origin in wave number space.

- The Gamma function. Look under
- (gamma) May indicate:
- Gyromagnetic ratio.
- Standard symbol for a photon of electromagnetic radiation.
- A nuclear de-excitation mode in which a photon is emitted.
- A nuclear vibrational mode that messes up the axial symmetry of the nucleus.
- Summation index.
- Integral in the tunneling WKB approximation.

- (capital delta) May indicate:
- An increment in the quantity following it.
- A delta particle.
- Often used to indicate the Laplacian
.

- (delta) May indicate:
- With two subscripts, the
Kronecker delta

, which by definition is equal to one if its two subscripts are equal, and zero in all other cases. - Without two subscripts, the “Dirac delta
function”, which is infinite when its argument is zero, and
zero if it is not. In addition the infinity is such that the
integral of the delta function over its single nonzero point is
unity. The delta function is not a normal function, but a
distribution. It is best to think of it as the approximate
function shown in the right hand side of figure 7.10 for a
very, very, small positive value of
. One often important way to create a three-dimensional delta function in spherical coordinates is to take the Laplacian of the function

1 /. Chapter 13.3 explains why. In two dimensions, take the Laplacian of/ to get a delta function. - Often used to indicate a small amount of the following
quantity, or of a small change in the following quantity. There
are nuanced differences in the usage of
, and that are too much to go in here. - Often used to indicate a second small quantity in addition to
.

- With two subscripts, the
- (partial) Indicates a vanishingly small
change or interval of the following variable. For example,
/ is the ratio of a vanishingly small change in functiondivided by the vanishingly small change in variable that causes this change in . Such ratios define derivatives, in this case the partial derivative ofwith respect to . Also used in relativistic index notation, chapter 1.2.5.

- (epsilon) May indicate:
is the permittivity of space. Equal to 8.854 187 817... 1 0 C/ J m. The exact value is1 1 0 C/ J m, because of the exact SI definitions of ampere and speed of light.- Scaled energy.
- Orbital energy.
- Lagrangian multiplier.
- A small quantity, if symbol
is not available.

- (variant of epsilon) May indicate:
- A very small quantity.
- The slop in energy conservation during a decay process.

- (eta) May be used to indicate a
- position of a particle. - (capital theta) Used in this book to
indicate some function of
to be determined. - (theta) May indicate:
- In spherical coordinates, the angle from the chosen
axis, with apex at the origin. - position of a particle.- A generic angle, like the one between the vectors in a cross or dot product.
- Integral acting as an angle in the classical WKB approximation.
- Integral acting as an angle in the adiabatic approximation.

- In spherical coordinates, the angle from the chosen
- (variant of theta) An alternate symbol
for
. - (kappa) May indicate:
- A constant that physically corresponds to some wave number.
- A summation index.
- Thermal conductivity.

- (Lambda) May indicate:
- Lorentz transformation matrix.

- (lambda) May indicate:
- Wave length.
- Decay constant.
- A generic eigenvalue.
- Entry of a Lorentz transformation.
- Scaled square momentum.
- Some multiple of something.

- (mu) May indicate:
- Magnetic dipole moment:

Alpha particle: 0 (spin is zero).

Deuteron: 0.433 073 49 10 J/T or 0.857 438 231.

Electron:9 .284 764 3 10 J/T or1 .001 159 652 180 8.

Helion:1 .074 617 49 10 J/T or2 .127 625 306.

Neutron:0 .966 236 5 10 J/T or1 .913 042 7.

Proton: 1.410 606 74 10 J/T or 2.792 847 36.

Triton: 1.504 609 45 10 J/T or 2.978 962 45. / 9.274 009 7 1 0 J/T or 5.788 381 807 10 eV/T is the Bohr magneton./ 5.050 783 5 1 0 J/T or 3.152 451 261 10 eV/T is the nuclear magneton.- A summation index.
- Chemical potential/molar Gibbs free energy.

- Magnetic dipole moment:
- (nu) May indicate:
- Electron neutrino.
- Scaled energy eigenfunction number in solids.
- A summation index.
- Strength of a delta function potential.

- (xi) May indicate:
- Scaled argument of the one-dimensional harmonic oscillator eigenfunctions.
- position of a particle.- A summation or integration index.

- (Oblique Pi) (Not to be confused with
described higher up.) Parity operator. Replaces by . That is equivalent to a mirroring in a mirror through the origin, followed by a 180 rotation around the axis normal to the mirror. - (pi) May indicate:
- A constant with value
3.141 592 653 589 793 238 462....

The area of a circle of radiusis and its perimeter is .

The volume of a sphere of radiusis and its surface is .

A 180 angle expressed in radians is.

Note also that1 and1. - A chemical bond that looks from the side like a p state.
- A particle involved in the forces keeping the nuclei of atoms
together
(- meson or pion for short). - Parity.

- A constant with value
3.141 592 653 589 793 238 462....
- Canonical momentum density.
- (rho) May indicate:
- Electric charge per unit volume.
- Scaled radial coordinate.
- Radial coordinate.
- Eigenfunction of a rotation operator
. - Mass-base density.
- Energy density of electromagnetic radiation.

- (sigma) May indicate:
- A standard deviation of a value.
- A chemical bond that looks like an s state when seen from the side.
- Pauli spin matrix.
- Surface tension.
- Electrical conductivity.
5.670 37 W/ m K is the Stefan-Boltzmann

- (tau) May indicate:
- A time or time interval.
- Life time or half life.
- Some coefficient.

- (capital phi) May indicate:
- Some function of
to be determined. - The momentum-space wave function.
- Relativistic electromagnetic potential.

- Some function of
- (phi) May indicate:
- In spherical coordinates, the angle around the chosen
axis. Increasing by encircles the - axis exactly once. - A phase angle.
- Something equivalent to an angle.
- Field operator
annihilates a particle at position while creates one at that position.

- In spherical coordinates, the angle around the chosen
- (variant of phi) May indicate:
- A change in angle
. - An alternate symbol for
. - An electrostatic potential.
- An electrostatic quantum field.
- A hypothetical selectostatic quantum field.

- A change in angle
- (chi) May indicate
- Spinor component.
- Gauge function of electromagnetic field.

- (capital psi) Upper case psi is used for the wave function.
- (psi) Typically used to indicate an energy
eigenfunction. Depending on the system, indices may be added to
distinguish different ones. In some cases
might be used instead of to indicate a system in an energy eigenstate. Let me know and I will change it. A system in an energy eigenstate should be written as , not, witha constant of magnitude 1. - (Omega) May indicate:
- Solid angle. See
angle

and “spherical coordinates.”

- Solid angle. See
- (omega) May indicate:
- Angular frequency of the classical harmonic oscillator. Equal
to
where is the spring constant and the mass. - Angular frequency of a system.
- Angular frequency of light waves.
- Perturbation frequency,
- Any quantity having units of frequency, 1/s.

- Angular frequency of the classical harmonic oscillator. Equal
to
- May indicate:
- Repeatedly used to indicate the operator for a generic
physical quantity
, with eigenfunctions. - Electromagnetic vector potential, or four vector potential.
- Einstein
coefficient. - Some generic matrix.
- Some constant.
- Area.

- Repeatedly used to indicate the operator for a generic
physical quantity
**Å**- Ångstrom. Equal to 1
0 m. - May indicate:
- The value of a generic physical quantity with operator
- The amplitude of the spin-up state
- The amplitude of the first state in a two-state system.
- Acceleration.
- Start point of an integration interval.
- The first of a pair of particles.
- Some coefficient.
- Some constant.
- Absorptivity of electromagnetic radiation.
- Annihilation operator
or creation operator . - Bohr radius of helium ion.

- The value of a generic physical quantity with operator
- May indicate:
- Bohr radius,
/ or 0.529 177 210 9 Å, with Å1 0 m. Comparable in size to atoms, and a good size to use to simplify various formulae. - The initial value of a coefficient
.

- Bohr radius,
**absolute**- May indicate:
- The absolute value of a real number
is indicated by . It equalsis is positive or zero and if is negative. - The absolute value of a complex number
is indicated by . It equals the length of the number plotted as a vector in the complex plane. This simplifies to above definition ifis real. - An absolute temperature is a temperature measured from
absolute zero. At absolute zero all systems are in their ground
state. Absolute zero is
2 73.15C in degrees Centrigrade (Celsius). The SI absolute temperature scale is degrees Kelvin, K. Absolute zero temperature is 0 K, while 0C is 273.15 K.

- The absolute value of a real number
**adiabatic**- An adiabatic process is a process in which there
is no heat transfer with the surroundings. If the process is also
reversible, it is called isentropic. Typically, these processes are
fairly quick, in order not to give heat conduction enough time to do
its stuff, but not so excessively quick that they become
irreversible.
Adiabatic processes in quantum mechanics are defined quite differently to keep students on their toes. See chapter 7.1.5. These processes are very slow, to give the system all possible time to adjust to its surroundings. Of course, quantum physicist were not aware that the same term had already been used for a hundred years or so for relatively fast processes. They assumed they had just invented a great new term!

**adjoint**- The adjoint
or of an operator is the one you get if you take it to the other side of an inner product. (While keeping the value of the inner product the same regardless of whatever two vectors or functions may be involved.) Hermitian operators are self-adjoint;

they do not change if you take them to the other side of an inner product.Skew-Hermitian

operators just change sign.Unitary operators

change into their inverse when taken to the other side of an inner product. Unitary operators generalize rotations of vectors: an inner product of vectors is the same whether you rotate the first vector one way, or the second vector the opposite way. Unitary operators preserve inner products (when applied to both vectors or functions). Fourier transforms are unitary operators on account of the Parseval equality that says that inner products are preserved. **amplitude**- Everything in quantum mechanics is an amplitude.
However, most importantly, the
quantum amplitude

gives the coefficient of a state in a wave function. For example, the usual quantum wave function gives the quantum amplitude that the particle is at the given position. **angle**- Consider two semi-infinite lines extending from a
common intersection point. Then the angle between these lines is
defined in the following way: draw a unit circle in the plane of the
lines and centered at their intersection point. The angle is then
the length of the circular arc that is in between the lines. More
precisely, this gives the angle in radians, rad. Sometimes an angle
is expressed in degrees, where
rad is taken to be 36 0. However, using degrees is usually a very bad idea in science.In three dimensions, you may be interested in the so-called

solid angle

inside a conical surface. This angle is defined in the following way: draw a sphere of unit radius centered at the apex of the conical surface. Then the solid angle is the area of the spherical surface that is inside the cone. Solid angles are in steradians. The cone does not need to be a circular one, (i.e. have a circular cross section), for this to apply. In fact, the most common case is the solid angle corresponding to an infinitesimal element of spherical coordinate system angles. In that case the surface of the unit sphere inside the conical surface is is approximately rectangular, with sides and . That makes the enclosed solid angle equal to. - May indicate:
- Repeatedly used to indicate a generic second operator or matrix.
- Einstein
coefficient. - Some constant.

- May indicate:
- Magnetic field strength.

- May indicate:
- Repeatedly used to indicate the amplitude of the spin-down state
- Repeatedly used to indicate the amplitude of the second state in a two-state system.
- End point of an integration interval.
- The second of a pair of particles.
- Some coefficient.
- Some constant.

**basis**- A basis is a minimal set of vectors or functions that
you can write all other vectors or functions in terms of. For
example, the unit vectors
, , andare a basis for normal three-dimensional space. Every three-dimensional vector can be written as a linear combination of the three. - May indicate:
- A third matrix or operator.
- A variety of different constants.

C - Degrees Centigrade. A commonly used
temperature scale that has the value
2 73.15C instead of zero when systems are in their ground state. Recommendation: use degrees Kelvin (K) instead. However, differences in temperature are the same in Centigrade as in Kelvin. - May indicate:
- The speed of light, 299 792 458 m/s exactly (by definition of the velocity unit).
- Speed of sound.
- Spring constant.
- A variety of different constants.

**Cauchy-Schwartz inequality**- The Cauchy-Schwartz inequality
describes a limitation on the magnitude of inner products. In
particular, it says that for any
and ,

In words, the magnitude of an inner productis at most the magnitude (i.e. the length or norm) of times the one of . For example, ifand are real vectors, the inner product is the dot product and you have , whereis the length of vector and the one of , andis the angle in between the two vectors. Since a cosine is less than one in magnitude, the Cauchy-Schwartz inequality is therefore true for vectors. But it is true even if

and are functions. To prove it, first recognize that may in general be a complex number, which according to (2.6) must take the form where is some real number whose value is not important, and that is its complex conjugate . Now, (yes, this is going to be some convoluted reasoning), look at

whereis any real number. The above dot product gives the square magnitude of , so it can never be negative. But if you multiply out, you get

and if this quadratic form inis never negative, its discriminant must be less or equal to zero:

and taking square roots gives the Cauchy-Schwartz inequality. **Classical**- Can mean any older theory. In this work, most of
the time it either means
nonquantum,

ornonrelativistic.

- The cosine function, a periodic function
oscillating between 1 and -1 as shown in
[41, pp. 40-]. See also
sin.

**curl**- The curl of a vector
is defined as . - May indicate:
- Difference in wave number values.

- Primitive (translation) vector of a reciprocal lattice.
- Density of states.
**D**- Often used to indicate a state with two units of orbital angular momentum.
- May indicate:
- The distance between the protons of a hydrogen molecule.
- The distance between the atoms or lattice points in a crystal.
- A constant.

- Primitive (translation) vector of a crystal lattice.
- Indicates a vanishingly small change or
interval of the following variable. For example,
can be thought of as a small segment of the - axis.In three dimensions,

is an infinitesimal volume element. The symbol means that you sum over all such infinitesimal volume elements. **derivative**- A derivative of a function is the ratio of a
vanishingly small change in a function divided by the vanishingly
small change in the independent variable that causes the change in
the function. The derivative of
with respect to is written as /, or also simply as. Note that the derivative of functionis again a function of : a ratiocan be found at every point . The derivative of a functionwith respect to is written as / to indicate that there are other variables,and , that do not vary. **determinant**- The determinant of a square matrix
is a single number indicated by . If this number is nonzero,can be any vector for the right choice of . Conversely, if the determinant is zero,can only produce a very limited set of vectors, though if it can produce a vector , it can do so for multiple vectors. There is a recursive algorithm that allows you to compute determinants from increasingly bigger matrices in terms of determinants of smaller matrices. For a 1

1 matrix consisting of a single number, the determinant is simply that number:

(This determinant should not be confused with the absolute value of the number, which is written the same way. Since you normally do not deal with 11 matrices, there is normally no confusion.) For 2 2 matrices, the determinant can be written in terms of 1 1 determinants:

so the determinant isin short. For 3 3 matrices, you have

and you already know how to work out those 22 determinants, so you now know how to do 3 3 determinants. Written out fully:

For 44 determinants,

Etcetera. Note the alternating sign pattern of the terms.As you might infer from the above, computing a good size determinant takes a large amount of work. Fortunately, it is possible to simplify the matrix to put zeros in suitable locations, and that can cut down the work of finding the determinant greatly. You are allowed to use the following manipulations without seriously affecting the computed determinant:

- You can
transpose

the matrix, i.e. change its columns into its rows. - You can create zeros in a row by subtracting a suitable multiple of another row.
- You can also swap rows, as long as you remember that each time that you swap two rows, it will flip over the sign of the computed determinant.
- You can also multiply an entire row by a constant, but that will multiply the computed determinant by the same constant.

for which is less than , and that makes evaluating the determinant pretty much trivial. - You can
**div(ergence)**- The divergence of a vector
is defined as . - May indicate:
- The total energy. Possible values are the eigenvalues of the Hamiltonian.
/ / / / may indicate the nonrelativistic (Bohr) energy levels of the hydrogen atom. The ground state energyequals -13.605 692 5 eV. This does not include relativistic and proton motion corrections. - Internal energy of a substance.

- May indicate:
- Electric field strength.

- May indicate:
- The basis for the natural logarithms. Equal to
2.718 281 828 459... This number produces the
exponential function

, or, or in words

, whose derivative with respect toto the power is again . Ifis a constant, then the derivative of is . Also, ifis an ordinary real number, then is a complex number with magnitude 1. - The magnitude of the charge of an electron or proton, equal to
1.602 176 57 1
0 C. - Emissivity of electromagnetic radiation.
- Often used to indicate a unit vector.
- A superscript
may indicate a single-electron quantity. - Specific internal energy of a substance.

- The basis for the natural logarithms. Equal to
2.718 281 828 459... This number produces the
**e**- May indicate
- Subscript e may indicate an electron.

- Assuming that
is an ordinary real number, and a real variable, is a complex function of magnitude one. The derivative of with respect to is **eigenvector**- A concept from linear algebra. A vector
is an eigenvector of a matrix if is nonzero and for some number called the corresponding eigenvalue. The basic quantum mechanics section of this book avoids linear algebra completely, and the advanced part almost completely. The few exceptions are almost all two-dimensional matrix eigenvalue problems. In case you did not have any linear algebra, here is the solution: the two-dimensional matrix eigenvalue problem

has eigenvalues that are the two roots of the quadratic equation

The corresponding eigenvectors are

On occasion you may have to swapand to use these formulae. If and are equal, there might not be two eigenvectors that are not multiples of each other; then the matrix is called defective. However, Hermitian matrices are never defective. See also

matrix” and “determinant.

**eV**- The electron volt, a commonly used unit of energy. Its
value is equal to 1.602 176 57 1
0 J. **exponential function**- A function of the form
, also written as. Seefunction

and. - May indicate:
- The force in Newtonian mechanics. Equal to the negative gradient of the potential. Quantum mechanics is formulated in terms of potentials, not forces.
- The anti-derivative of some function
. - Some function.
- Helmholtz free energy.

- Fock operator.
- May indicate:
- A generic function.
- A generic vector.
- A fraction.
- The resonance factor.
- Specific Helmholtz free energy.
- Frequency.

**function**- A mathematical object that associates values with
other values. A function
associates every value of with a value . For example, the functionassociates 0 with 0, with , 1 with 1, 2 with 4, 3 with 9, and more generally, any arbitrary value of with the square of that value . Similarly, functionassociates any arbitrary with its cube , associates any arbitrary with the sine of that value, etcetera. One way of thinking of a function is as a procedure that allows you, whenever given a number, to compute another number.

A wave function

associates each spatial position with a wave function value. Going beyond mathematics, its square magnitude associates any spatial position with the relative probability of finding the particle near there. **functional**- A functional associates entire functions with single numbers. For example, the expectation energy is mathematically a functional: it associates any arbitrary wave function with a number: the value of the expectation energy if physics is described by that wave function.
- May indicate:
- Gibbs free energy.
- Newton’s constant of gravitation, 6.673 8 1
0 m/ kgs.

- May indicate:
- A second generic function or a second generic vector.
- The strength of gravity, by definition equal to 9.806 65
m/
s exactly under standard conditions on the surface of the earth. - The g-factor, a nondimensional constant that indicates the
gyromagnetic ratio relative to charge and mass. For the electron
2 .002 319 304 361 5. For the proton5.585 694 71. For the neutron, based on the mass and charge of the proton, 3 .826 085 5. - Specific Gibbs free energy/chemical potential.

**Gauss' Theorem**- This theorem, also called divergence theorem
or Gauss-Ostrogradsky theorem, says that for a continuously
differentiable vector
,

where the first integral is over the volume of an arbitrary region and the second integral is over all the surface area of that region;is at each point found as the unit vector that is normal to the surface at that point. **grad(ient)**- The gradient of a scalar
is defined as . - May indicate:
- The Hamiltonian, or total energy, operator. Its eigenvalues
are indicated by
. stands for the - th order Hermite polynomial.- Enthalpy.

- The Hamiltonian, or total energy, operator. Its eigenvalues
are indicated by
- May indicate:
- The original Planck constant
. is a one-dimensional harmonic oscillator eigenfunction. - Single-electron Hamiltonian.
- Specific enthalpy.

- The original Planck constant
- The reduced Planck constant, equal to
1.054 571 73 1
0 J s. A measure of the uncertainty of nature in quantum mechanics. Multiply byto get the original Planck constant . For nuclear physics, a frequently helpful value is197.326 972 MeV fm. **hypersphere**- A hypersphere is the generalization of the
normal three-dimensional sphere to
- dimensional space. A sphere of radiusin three-dimensional space consists of all points satisfying

where, , andare Cartesian coordinates with origin at the center of the sphere. Similarly a hypersphere in - dimensional space is defined as all points satisfying

So a two-dimensionalhypersphere

of radiusis really just a circle of radius . A one-dimensionalhypersphere

is really just the line segment. The

volume”

and surface “area of an - dimensional hypersphere is given by

(This is readily derived recursively. For a sphere of unit radius, note that the- dimensionalvolume

is an integration of- dimensional volumes with respect to. Then renotateas and look up the resulting integral in a table book. The formula for the area follows because where is the distance from the origin.) In three dimensions, according to the above formula. That makes the three-dimensional volume

3 equal to the actual volume of the sphere, and the three-dimensional area

equal to the actual surface area. On the other hand in two dimensions, . That makes the two-dimensionalvolume

really the area of the circle. Similarly the two-dimensional surface area

is really the perimeter of the circle. In one dimensions and the volume

is really the length of the interval, and the area

2 is really its number of end points.Often the infinitesimal

- dimensionalvolume

elementis needed. This is the infinitesimal integration element for integration over all coordinates. It is:

Specifically, in two dimensions:

while in three dimensions:

The expressions in parentheses arein polar coordinates, respectively in spherical coordinates. - May indicate:
- The number of electrons or particles.
- Electrical current.
- Unit matrix or operator, which does not do anything. See
matrix.

is Avogadro’s number, 6.022 141 3 1 0 particles per kmol. (More standard symbols areor , but they are incompatible with the general notations in this book.)

- The imaginary part of a complex number. If
with and real numbers, then . Note that. - May indicate:
is radiation energy intensity. is moment of inertia.

- May indicate:
- The number of a particle.
- A summation index.
- A generic index or counter.

. - The unit vector in the
- direction. - The standard square root of minus one:
, 1 , 1/, . **index notation**- A more concise and powerful way of writing
vector and matrix components by using a numerical index to indicate
the components. For Cartesian coordinates, you might number the
coordinates
as 1, as 2, and as 3. In that case, a sum like can be more concisely written as . And a statement like0, 0, 0 can be more compactly written as 0. To really see how it simplifies the notations, have a look at the matrix entry. (And that one shows only 2 by 2 matrices. Just imagine 100 by 100 matrices.) **iff**- Emphatic
if.

Should be read asif and only if.

**integer**- Integer numbers are the whole numbers:
. **inverse**- (Of matrices or operators.) If an operator
converts a vector or function into a vector or function , then the inverse of the operatorconverts back into . For example, the operator 2 converts vectors or functions into two times themselves, and its inverse operatorconverts these back into the originals. Some operators do not have inverses. For example, the operator 0 converts all vectors or functions into zero. But given zero, there is no way to figure out what function or vector it came from; the inverse operator does not exist. **irrotational**- A vector
is irrotational if its curl is zero. **iso**- Means
equal” or “constant.

- Isenthalpic: constant enthalpy.
- Isentropic: constant entropy. This is a process that is both adiabatic and reversible.
- Isobaric: constant pressure.
- Isochoric: constant (specific) volume.
- Isospin: you don’t want to know.
- Isothermal: constant temperature.

**isolated**- An isolated system is one that does not interact with its surroundings in any way. No heat is transfered with the surroundings, no work is done on or by the surroundings.
- May indicate:
- Total angular momentum.
- Number of nuclei in a quantum computation of electronic structure.

- May indicate:
- The azimuthal quantum number of total angular momentum, including both orbital and spin contributions.
is electric current density. - The number of a nucleus in a quantum computation.
- A summation index.
- A generic index or counter.

- The unit vector in the
- direction. - May indicate:
- An exchange integral in Hartree-Fock.
- Maximum wave number value.

- Thomson (Kelvin) coefficient.
**K**- May indicate:
- The atomic states or orbitals with theoretical Bohr energy
- Degrees Kelvin.

- The atomic states or orbitals with theoretical Bohr energy
- May indicate:
- A wave number. A wave number is a measure for how fast a
periodic function oscillates with variations in spatial position.
In quantum mechanics,
is normally defined as /. The vectoris not to be confused with the unit vector in the - direction. - A generic summation index.

- A wave number. A wave number is a measure for how fast a
periodic function oscillates with variations in spatial position.
In quantum mechanics,
- The unit vector in the
- direction. - Boltzmann constant. Equal to
1.380 649 1
0 J/K. Relates absolute temperature to a typical unit of heat motion energy. **kmol**- A kilo mole refers to 6.022 141 3 1
0 atoms or molecules. The weight of this many particles is about the number of protons and neutrons in the atom nucleus/molecule nuclei. So a kmol of hydrogen atoms has a mass of about 1 kg, and a kmol of hydrogen molecules about 2 kg. A kmol of helium atoms has a mass of about 4 kg, since helium has two protons and two neutrons in its nucleus. These numbers are not very accurate, not just because the electron masses are ignored, and the free neutron and proton masses are somewhat different, but also because of relativity effects that cause actual nuclear masses to deviate from the sum of the free proton and neutron masses. - May indicate:
- Angular momentum.
- Orbital angular momentum.

- Lagrangian.
**L**- The atomic states or orbitals with theoretical Bohr energy
- May indicate:
- The azimuthal quantum number of angular momentum.
- The azimuthal quantum number of orbital angular momentum.
Here
is used for spin, and for combined angular momentum.) - A generic summation index.

- May indicate:
- The typical length in the harmonic oscillator problem.
- The dimensions of a solid block (with subscripts).
- A length.
- Multipole level in transitions.

- Lagrangian density. This is best understood in the UK.
- Indicates the final result of an approaching
process.
indicates for practical purposes the value of the following expression when is extremely small. **linear combination**- A very generic concept indicating sums of
objects times coefficients. For example, a position vector
in basic physics is the linear combination with the objects the unit vectors , , andand the coefficients the position coordinates , , and. A linear combination of a set of functionswould be the function

whereare constants, i.e. independent of . **linear dependence**- A set of vectors or functions is linearly
dependent if at least one of the set can be expressed in terms of
the others. Consider the example of a set of functions
. This set is linearly dependent if

where at least one of the constantsis nonzero. To see why, suppose that say is nonzero. Then you can divide by and rearrange to get

That expressesin terms of the other functions. **linear independence**- A set of vectors or functions is
linearly independent if none of the set can be expressed in terms of
the others. Consider the example of a set of functions
. This set is linearly independent if

only if every one of the constantsis zero. To see why, assume that say could be expressed in terms of the others,

Then taking1, , , ..., the condition above would be violated. Socannot be expressed in terms of the others. - May indicate:
- Molecular mass. See
molecular mass.

- Figure of merit.

- Molecular mass. See
- Mirror operator.
**M**- The atomic states or orbitals with theoretical Bohr energy
- May indicate:
- Mass.
: electron mass. Equal to 9.109 382 9 10 kg. The rest mass energy is 0.510 998 93 MeV.: proton mass. Equal to 1.672 621 78 10 kg. The rest mass energy is 938.272 013 MeV.: neutron mass. Equal to 1.674 927 10 kg. The rest mass energy is 939.565 561 MeV.- Alpha particle: 6.644 656 8 1
0 kg or 3 727.379 24 MeV.

Deuteron: 3.343 583 5 10 kg or 1 875.612 86 MeV.

Helion: 5.006 412 3 10 kg or 2 808.391 482 MeV. 1.660 538 92 1 0 kg is the atomic mass constant.: generic particle mass.

- The magnetic quantum number of angular momentum. The type odf
angular momentum may be indicated by a subscript
for orbital, for spin, or for net (orbital plus spin). - Number of a single-electron wave function.
- Number of rows in a matrix.
- A generic summation index or generic integer.

- Mass.
**matrix**- A table of numbers.
As a simple example, a two-dimensional (or

) matrixis a table of four numbers called , , , and:

unlike a two-dimensional vector, which would consist of only two numbersand arranged in a column:

(Such a vector can be seen as arectangular matrix

of size 21, but let’s not get into that.) (Note that in quantum mechanics, if a vector is written as a column, considered the normal case, it is called a ket

vector. If the complex conjugates of its numbers are written as a row, it is called abra

vector.)In

index notation,

a matrixis a set of numbers, or coefficients,

indexed by two indices. The first index is the row number at which the coefficient is found in matrix , and the second indexis the column number. In index notation, a matrix turns a vector into another vector according to the recipe

wherestands for “the - th component of vector, ” andfor “the - th component of vector. ”As an example, the product of

and above is by definition

which is just another two-dimensional ket vector.Note that in matrix multiplications, like in the example above, in geometric terms you take dot products between the rows of the first factor and the columns of the second factor.

To multiply two matrices together, just think of the columns of the second matrix as separate vectors. For example, to multiply two

matrices and together:

which is another two-dimensional matrix.(Note that you cannot normally swap the order of matric multiplication. The matrix

is different from matrix . In the special case thatand are the same and and have complete sets of eigenvectors, then they have a common complete set of eigenvectors, {D.18}.) In index notation, if

, then each coefficientof matrix is given in terms of the coefficients of and as

Note that the indexthat you sum over is the second of but the first of . In short, you sum over “neighboring indices.” Since you sum over all, the result does not depend on. The zero matrix, usually called

, is like the number zero; it does not change a matrix it is added to. And it turns whatever it is multiplied with into zero. A zero matrix has every coefficient zero. For example, in two dimensions:

A unit, or identity, matrix, usually called

, is the equivalent of the number one for matrices; it does not change the vector or matrix it is multiplied with. A unit matrix is one on itsmain diagonal

and zero elsewhere. The 2 by 2 unit matrix is:

More generally the coefficients,, of a unit matrix are one ifand zero otherwise. The

transpose

of a matrix, , is what you get if you swap the two indices. Graphically, it turns its rows into its columns and vice versa. Theadjoint

orHermitian adjoint

matrixis what you get if you both swap the two indices in a matrix and then take the complex conjugate of every coefficient. If you want to take a matrix to the other side of an inner product, you will need to change it to its Hermitian adjoint. Hermitian matrices

are equal to their Hermitian adjoint, so this does nothing for them.The inverse of a matrix

, is a matrix so that equals the identity matrix . That is much like the inverse of a simple number times that number gives one. And, just like the number zero has no inverse, a matrix with zero determinant has no inverse. Otherwise, you can swap the order;equals the unit matrix too. (For numbers this is trivial, for matrices you need to look a bit closer to understand why it is true.) See also

determinant

andeigenvector.

**metric prefixes**- In the metric system, the prefixes Y, Z, E,
P, T, G, M, and k stand for 1
0 with24, 21, 18, 15, 12, 9, 6, and 3, respectively. Similarly, d, c, m, , n, p, f, a, z, y stand for 10 with1, 2, 3, 6, 9, 12, 15, 18, 21, and 24 respectively. For example, 1 ns is 1 0 seconds. English letter u is often used as instead of greek. Names corresponding to the mentioned prefixes Y-k are yotta, zetta, exa, peta, tera, giga, mega, kilo, and corresponding to d-y are deci, centi, milli, micro, nano, pico, femto, atto, zepto, and yocto. **molecular mass**- Typical thermodynamics books for engineers
tabulate values of the
molecular mass,

as a nondimensional number. The bottom line first: these numbers should have been called themolar mass

of the substance, for the naturally occurring isotope ratio on earth. And they should have been given units of kg/kmol. That is how you use these numbers in actual computations. So just ignore the fact that what these books really tabulate is officially called therelative molecular mass

for the natural isotope ratio.Don’t blame these textbooks too much for making a mess of things. Physicists have historically bandied about a zillion different names for what is essentially a single number. Like

molecular mass,

“relative molecular mass,”molecular weight,

“atomic mass,”relative atomic mass,

“atomic weight,”molar mass,

“relative molar mass,” etcetera are basically all the same thing.All of these have values that equal the mass of a molecule relative to a reference value for a single nucleon. So these value are about equal to the number of nucleons (protons and neutrons) in the nuclei of a single molecule. (For an isotope ratio, that becomes the average number of nucleons. Do note that nuclei are sufficiently relativistic that a proton or neutron can be noticeably heavier in one nucleus than another, and that neutrons are a bit heavier than protons even in isolation.) The official reference nucleon weight is defined based on the most common carbon isotope carbon-12. Since carbon-12 has 6 protons plus 6 neutrons, the reference nucleon weight is taken to be one twelfth of the carbon-12 atomic weight. That is called the unified atomic mass unit (u) or Dalton (Da). The atomic mass unit (amu) is an older virtually identical unit, but physicists and chemists could never quite agree on what its value was. No kidding.

If you want to be politically correct, the deal is as follows.

Molecular mass

is just what the term says, the mass of a molecule, in mass units. (I found zero evidence in either the IUPAC Gold Book or NIST SP811 for the claim of Wikipedia that it must always be expressed in u.)Molar mass

is just what the words says, the mass of a mole. Official SI units are kg/mol, but you will find it in g/mol, equivalent to kg/kmol. (You cannot expect enough brains from international committees to realize that if you define the kg and not the g as unit of mass, then it would be a smart idea to also define kmol instead of mol as unit of particle count.) Simply ignore relative atomic and molecular masses, you do not care about them. (I found zero evidence in either the IUPAC Gold Book or NIST SP811 for the claims of Wikipedia that the molecular mass cannot be an average over isotopes or that the molar mass must be for a natural isotope ratio. In fact, NIST usesmolar mass of carbon-12

and specifically includes the possibility of an average in the relative molecular mass.)See also the atomic mass constant

. - May indicate:
- Number of states.
- Number of single-particle states.
- Number of neutrons in a nucleus.

**N**- May indicate
- The atomic states or orbitals with theoretical Bohr energy
. - Subscript N indicates a nucleus.

- The atomic states or orbitals with theoretical Bohr energy
- May indicate:
- The principal quantum number for hydrogen atom energy eigenfunctions.
- A quantum number for harmonic oscillator energy eigenfunctions.
- Number of a single-electron or single-particle wave function.
- Generic summation index over energy eigenfunctions.
- Generic summation index over other eigenfunctions.
- Integer factor in Fourier wave numbers.
- Probability density.
- Number of columns in a matrix.
- A generic summation index or generic integer.
- A natural number.
is the number of spin states.

**n**- May indicate
- A subscript n may indicate a neutron.

**natural**- Natural numbers are the numbers:
. **normal**- A normal operator or matrix is one that has
orthonormal eigenfunctions or eigenvectors. Since eigenvectors are
not orthonormal in general, a normal operator or matrix is abnormal!
Another example of a highly confusing term. Such a matrix should
have been called orthodiagonalizable or something of the kind. To
be fair, the author is not aware of any physicists being involved in
this particular term; it may be the mathematicians that are to blame
here.
For an operator or matrix

to be normal,

it must commute with its Hermitian adjoint,0. Hermitian matrices are normal since they are equal to their Hermitian adjoint. Skew-Hermitian matrices are normal since they are equal to the negative of their Hermitian adjoint. Unitary matrices are normal because they are the inverse of their Hermitian adjoint. **O**- May indicate the origin of the coordinate system.
**opposite**- The opposite of a number
is . In other words, it is the additive inverse. - May indicate:
- The linear momentum eigenfunction.
- A power series solution.
- Probability.
- Pressure.
- Hermitian part of an annihilation operator.

- Particle exchange operator. Exchanges the positions and spins of two identical particles.
- Peltier coefficient.
**P**- Often used to indicate a state with one unit of orbital angular momentum.
- May indicate:
- Linear momentum.
- Linear momentum in the
- direction. - Integration variable with units of linear momentum.

**p**- May indicate
- An energy state with orbital azimuthal quantum number
1. - A superscript p may indicate a single-particle quantity.
- A subscript p may indicate a periodic function.
- A subscript p may indicate a proton.

- An energy state with orbital azimuthal quantum number
**perpendicular bisector**- For two given points
and , the perpendicular bisector consists of all pointsthat are equally far from as they are from . In two dimensions, the perpendicular bisector is the line that passes through the point exactly half way in betweenand , and that is orthogonal to the line connectingand . In three dimensions, the perpendicular bisector is the plane that passes through the point exactly half way in betweenand , and that is orthogonal to the line connectingand . In vector notation, the perpendicular bisector of pointsand is all points whose radius vector satisfies the equation:

(Note that the halfway pointis included in this formula, as is the half way point plus any vector that is normal to . ) **phase angle**- Any complex number can be written in
polar form

aswhere both the magnitude and the phase angle are real numbers. Note that when the phase angle varies from zero to , the complex numbervaries from positive real to positive imaginary to negative real to negative imaginary and back to positive real. When the complex number is plotted in the complex plane, the phase angle is the direction of the number relative to the origin. The phase angle is often called the argument, but so is about everything else in mathematics, so that is not very helpful. In complex time-dependent waves of the form

, and its real equivalent, the phase anglegives the angular argument of the wave at time zero. **photon**- Unit of electromagnetic radiation (which includes
light, x-rays, microwaves, etcetera). A photon has a energy
, whereis its angular frequency, and a wave length / whereis the speed of light. **potential**- In order to optimize confusion, pretty much everything in physics that is scalar is called potential. Potential energy is routinely concisely referred to as potential. It is the energy that a particle can pick up from a force field by changing its position. It is in Joule. But an electric potential is taken to be per unit charge, which gives it units of volts. Then there are thermodynamic potentials like the chemical potential.
- Linear momentum in the
- direction. (In the one-dimensional cases at the end of the unsteady evolution chapter, thesubscript is omitted.) Components in the - and- directions areand . Classical Newtonian physics haswhere is the mass and the velocity in the - direction. In quantum mechanics, the possible values ofare the eigenvalues of the operator which equals /. (But which becomes canonical momentum in a magnetic field.) - May indicate
- Number of energy eigenfunctions of a system of particles.
- Anti-Hermitian part of an annihilation operator divided by
. - Heat flow or heat.
- Charge.
- Electric quadrupole moment.
- Energy release.

- May indicate:
- Charge.
- Heat flux density.
- The number of an energy eigenfunction of a system of particles.
- Generic index.

- May indicate:
- Ideal gas constant.
- Transition rate.
- Nuclear radius.
- Reflection coefficient.
- Some radius or typical radius (like in the Yukawa potential).
- Some function of
to be determined. - Some function of
to be determined. is a hydrogen radial wave function. 8.314 462 kJ/kmol K is the universal gas constant. It is the equivalent of Boltzmann's constant, but for a kmol instead of a single atom or molecule.

- Rotation operator.
- The real part of a complex number. If
with and real numbers, then . Note that. - May indicate:
- The radial distance from the chosen origin of the coordinate system.
typically indicates the - th Cartesian component of the radius vector. - Some ratio.

- The position vector. In Cartesian coordinates
or . In spherical coordinates. Its three Cartesian components may be indicated byor by or by . **reciprocal**- The reciprocal of a number
is 1/ . In other words, it is the multiplicative inverse. **relativity**- The special theory of relativity accounts for the
experimental observation that the speed of light
is the same in all local coordinate systems. It necessarily drops the basic concepts of absolute time and length that were corner stones in Newtonian physics. Albert Einstein should be credited with the boldness to squarely face up to the unavoidable where others wavered. However, he should also be credited for the boldness of swiping the basic ideas from Lorentz and Poincaré without giving them proper, or any, credit. The evidence is very strong he was aware of both works, and his various arguments are almost carbon copies of those of Poincaré, but in his paper it looks like it all came from Einstein, with the existence of the earlier works not mentioned. (Note that the general theory of relativity, which is of no interest to this book, is almost surely properly credited to Einstein. But he was a lot less hungry then.)

Relativity implies that a length seen by an observer moving at a speed

is shorter than the one seen by a stationary observer by a factor assuming the length is in the direction of motion. This is called Lorentz-Fitzgerald contraction. It makes galactic travel somewhat more conceivable because the size of the galaxy will contract for an astronaut in a rocket ship moving close to the speed of light. Relativity also implies that the time that an event takes seems to be slower by a factor if the event is seen by an observer in motion compared to the location where the event occurs. That is called time dilation. Some high-energy particles generated in space move so fast that they reach the surface of the earth though this takes much more time than the particles would last at rest in a laboratory. The decay time increases because of the motion of the particles. (Of course, as far as the particles themselves see it, the distance to travel is a lot shorter than it seems to be to earth. For them, it is a matter of length contraction.) The following formulae give the relativistic mass, momentum, and kinetic energy of a particle in motion:

whereis the rest mass of the particle, i.e. the mass as measured by an observer to whom the particle seems at rest. The formula for kinetic energy reflects the fact that even if a particle is at rest, it still has an amount of build-in

energy equal toleft. The total energy of a particle in empty space, being kinetic and rest mass energy, is given by

as can be verified by substituting in the expression for the momentum, in terms of the rest mass, and then taking both terms inside the square root under a common denominator. For small linear momentum, this can be approximated as. Relativity seemed quite a dramatic departure of Newtonian physics when it developed. Then quantum mechanics started to emerge...

**rot**- The rot of a vector
is defined as . - May indicate:
- Number of states per unit volume.
- Number of states at a given energy level.
- Spin angular momentum (as an alternative to using
or for generic angular momentum.) - Entropy.
is a factor in the so-called tensor potential of nucleons.

- The action integral of Lagrangian mechanics, {A.1}
- Seebeck coefficient.
**S**- Often used to indicate a state of zero orbital angular momentum.
- May indicate:
- Spin value of a particle. Equals
for electrons, protons, and neutrons, is also half an odd natural number for other fermions, and is a nonnegative integer for bosons. It is the azimuthal quantum number due to spin. - Specific entropy.
- As an index, shelf number.

- Spin value of a particle. Equals
**s**- May indicate:
- An energy state with orbital azimuthal quantum number
0. Such a state is spherically symmetric.

- An energy state with orbital azimuthal quantum number
**scalar**- A quantity that is not a vector, a quantity that is just a single number.
- The sine function, a periodic function
oscillating between 1 and -1 as shown in
[41, pp. 40-]. Good to remember:
1 and and . **solenoidal**- A vector
is solenoidal if its divergence is zero. **spectrum**- In this book, a spectrum normally means a plot of
energy levels along the vertical axis. Often, the horizontal
coordinate is used to indicate a second variable, such as the
density of states or the particle velocity.
For light (photons), a spectrum can be obtained experimentally by sending the light through a prism. This separates the colors in the light, and each color means a particular energy of the photons.

The word spectrum is also often used in a more general mathematical sense, but not in this book as far as I can remember.

**spherical coordinates**- The spherical coordinates
, , andof an arbitrary point P are defined as In Cartesian coordinates, the unit vectors in the

, , anddirections are called , , and. Similarly, in spherical coordinates, the unit vectors in the, , anddirections are called , , and. Here, say, thedirection is defined as the direction of the change in position if you increase by an infinitesimally small amount while keeping and the same. Note therefore in particular that the direction of is the same as that of ; radially outward.An arbitrary vector

can be decomposed in components , , andalong these unit vectors. In particular

Recall from calculus that in spherical coordinates, a volume integral of an arbitrary function

takes the form

In other words, the volume element in spherical coordinates is

Often it is convenient of think of volume integrations as a two-step process: first perform an integration over the angular coordinatesand . Physically, that integrates over spherical surfaces. Then perform an integration overto integrate all the spherical surfaces together. The combined infinitesimal angular integration element

is called the infinitesimalsolid angle

. In two-dimensional polar coordinatesand , the equivalent would be the infinitesimal polar angle. Recall that, (in proper radians of course), equals the arclength of an infinitesimal part of the circle of integration divided by the circle radius. Similarlyis the surface of an infinitesimal part of the sphere of integration divided by the square sphere radius. See the

entry for the gradient operator and Laplacian in spherical coordinates. **Stokes' Theorem**- This theorem, first derived by Kelvin and
first published by someone else I cannot recall, says that for any
reasonably smoothly varying vector
,

where the first integral is over any smooth surface areaand the second integral is over the edge of that surface. How did Stokes get his name on it? He tortured his students with it, that’s how! One important consequence of the Stokes theorem is for vector fields

that are irrotational,

i.e. that have0. Such fields can be written as

Hereis the position of an arbitrarily chosen reference point, usually the origin. The reason the field can be written this way is the Stokes theorem. Because of the theorem, it does not make a difference along which path from to you integrate. (Any two paths give the same answer, as long as is irrotational everywhere in between the paths.) So the definition of is unambiguous. And you can verify that the partial derivatives of give the components of by approaching the final position in the integration from the corresponding direction. **symmetry**- A symmetry is an operation under which an object does not change. For example, a human face is almost, but not completely, mirror symmetric: it looks almost the same in a mirror as when seen directly. The electrical field of a single point charge is spherically symmetric; it looks the same from whatever angle you look at it, just like a sphere does. A simple smooth glass (like a glass of water) is cylindrically symmetric; it looks the same whatever way you rotate it around its vertical axis.
- May indicate:
- Absolute temperature. The absolute temperature in degrees K
equals the temperature in centigrade plus 273.15. When the
absolute temperature is zero, (i.e. at
2 73.15C ), nature is in the state of lowest possible energy. - Kinetic energy. A hat indicates the associated operator. The
operator is given by the Laplacian times
/. - Isospin. A hat indicates the associated operator. A vector symbol or subscript distinguishes it from kinetic energy.
- Tesla. The unit of magnetic field strength, kg/C-s.

- Absolute temperature. The absolute temperature in degrees K
equals the temperature in centigrade plus 273.15. When the
absolute temperature is zero, (i.e. at
- Translation operator that translates a wave function through space. The amount of translation is usually indicated by a subscript.
- May indicate:
- Time.
is the quantum number of square isospin.

**temperature**- A measure of the heat motion of the particles
making up macroscopic objects. At absolute zero temperature, the
particles are in the
ground state

of lowest possible energy. **triple product**- A product of three vectors. There are two
different versions:
- The scalar triple product
. In index notation,

whereis the index following in the sequence 123123..., and the one preceding it. This triple product equals the determinant formed with the three vectors. Geometrically, it is plus or minus the volume of the parallelepiped that has vectors , , andas edges. Either way, as long as the vectors are normal vectors and not operators,

and you can change the two sides of the dot product without changing the triple product, and/or you can change the sides in the vectorial product with a change of sign. If any of the vectors is an operator, use the index notation expression to work it out. - The vectorial triple product
. In index notation, component numberof this triple product is

which may be rewritten as

In particular, as long as the vectors are normal ones,

- The scalar triple product
- May indicate:
- A unitary operator, in other words one that does not change the magnitude of the wave function.
- Often used for energy, though not in this book.

- The time shift operator:
changes the wave function into . If the Hamiltonian is independent of time

- May indicate:
- The first velocity component in a Cartesian coordinate system.
- A complex coordinate in the derivation of spherical harmonics.
- An integration variable.

**u**- May indicate the atomic mass constant, equivalent to
1.660 538 92 1
0 kg or 931.494 06 MeV/. - May indicate:
- The potential energy.
is used interchangeably for the numerical values of the potential energy and for the operator that corresponds to multiplying by . In other words,is simply written as .

- The potential energy.
- Volume.
- May indicate:
- The second velocity component in a Cartesian coordinate system.
- Magnitude of a velocity (speed).
is specific volume. - A complex coordinate in the derivation of spherical harmonics.
- As
, a single electron pair potential.

- May indicate:
- Velocity vector.
- Generic vector.
- Summation index of a lattice potential.

**vector**- Simply put, a list of numbers. A vector
in index notation is a set of numbers indexed by an index . In normal three-dimensional Cartesian space,takes the values 1, 2, and 3, making the vector a list of three numbers, , , and. These numbers are called the three components of. The list of numbers can be visualized as a column, and is then called a ket vector, or as a row, in which case it is called a bra vector. This convention indicates how multiplication should be conducted with them. A bra times a ket produces a single number, the dot product or inner product of the vectors:

To turn a ket into a bra for purposes of taking inner products, write the complex conjugates of its components as a row.Formal definitions of vectors vary, but real mathematicians will tell you that vectors are objects that can be manipulated in certain ways (addition and multiplication by a scalar). Some physicists define vectors as objects that transform in a certain way under coordinate transformation (one-dimensional tensors); that is not the same thing.

**vectorial product**- An vectorial product, or cross product is a product of vectors
that produces another vector. If

it means in index notation that the- th component of vectoris

whereis the index following in the sequence 123123..., and the one preceding it. For example, will equal . **W**- May indicate:
- Watt, the SI unit of power.
- The
W are the charged carriers of the weak force. See alsoZ. - W.u. stands for Weisskopf unit, a simple decay ballpark for gamma decay.

- May indicate:
- The third velocity component in a Cartesian coordinate system.
- Weight factor.

- Generic vector.
- Used in this book to indicate a function of
to be determined. - May indicate:
- First coordinate in a Cartesian coordinate system.
- A generic argument of a function.
- An unknown value.

- Used in this book to indicate a function of
to be determined. - Spherical harmonic. Eigenfunction of both
angular momentum in the
- direction and of total square angular momentum. - May indicate:
- Second coordinate in a Cartesian coordinate system.
- A second generic argument of a function.
- A second unknown value.

- May indicate:
- Atomic number (number of protons in the nucleus).
- Number of particles.
- Partition function.
- The
Z is the uncharged carrier of the weak force. See alsoW. - Used in this book to indicate a function of
to be determined.

- May indicate:
- Third coordinate in a Cartesian coordinate system.
- A third generic argument of a function.
- A third unknown value.