CHEM2524Chemical Physics

    Glossary

    Every term and acronym the unit uses, in one alphabetical list.

    250 of 250 terms

    Absolute zero

    The temperature at which every molecule is in the ground state. There is no lower energy, so no lower temperature.

    • statistical mechanics
    • thermodynamics
    Accessible volume

    The space available to the centre of a particle. The more room it has, the more arrangements it can take, and the more entropy.

    • module-8
    • liquid crystals
    Activation energyE_a

    The energy an ion or molecule needs to get over a barrier, such as an ion hopping to the next lattice site.

    • module-6
    • kinetics
    Amorphous

    Without the long-range regular order of a crystal.

    • module-7
    • glasses
    Amphiphile

    A molecule with one end that likes the solvent and one end that avoids it, such as a charged head and a fatty tail. At high concentration these molecules clump so the tails hide.

    • module-8
    • liquid crystals
    Anisotropy

    Properties that depend on the direction you measure. The opposite of isotropic, where every direction looks the same.

    • module-8
    • liquid crystals
    Antiferromagnetism

    Neighbouring spins point opposite ways and cancel, so there is no net magnetisation at zero field.

    • module-3
    • magnetism
    Antifluorite

    Li2O type. ccp anions with all tetrahedral holes filled by cations. Coordination 4:8.

    • module-2
    • ionic
    Arrhenius equation

    A rate or conductivity that grows as exp(-E_a/kT): rising temperature makes it climb fast, a bigger barrier makes it small.

    • module-6
    • kinetics
    Band

    A strip of allowed electron energies. In a crystal the orbitals of many atoms sit so close together that they blur into one continuous band.

    • module-3
    • band theory
    Band gap

    The energy difference between the highest occupied state in the valence band and the lowest unoccupied state in the conduction band. Semiconductors are about 0.5 to 3 eV.

    • module-3
    • band theory
    BCS theoryBardeen-Cooper-Schrieffer theory

    The quantum theory of superconductivity as electron pairing. It gives k_B T_c = hbar omega exp(-1/(V N(E_f))).

    • module-3
    • superconductivity
    Betaβ = 1/kT

    The one number that sets all the populations. The lecture defines temperature so that beta is 1 over kT.

    • statistical mechanics
    Birefringence

    When light shaking in two directions travels at two different speeds through an aligned material, so the two parts drift out of step.

    • module-8
    • optics
    Bohr magnetonmu_B

    The unit of an electron magnetic moment, 9.27 x 10^-24 A m^2.

    • module-3
    • magnetism
    Boltzmann constantk

    The constant that links energy to temperature, exactly 1.380649 x 10^-23 J per kelvin.

    • statistical mechanics
    Boltzmann distribution

    The share of molecules in each energy level at equilibrium. Higher levels hold exponentially fewer molecules.

    • statistical mechanics
    Bomb calorimeter

    A sealed steel container sitting in water, used to measure heat at constant volume.

    • module-7
    • calorimetry
    Born–Mayer equation

    Gives lattice enthalpy from the ion charges, the ion separation d, a repulsion constant d* and the Madelung constant.

    • module-2
    • ionic
    Bragg equationn lambda = 2 d sin theta

    Links the X-ray wavelength, the spacing between planes and the angle at which reflections appear.

    • module-2
    • diffraction
    Bravais lattice

    One of 14 distinct lattices, made from the seven crystal systems with primitive (P), base-centred (C), body-centred (I) or face-centred (F) centring.

    • module-2
    • crystals
    Caesium chloride structure

    Two interpenetrating simple cubic cells, not close-packed. Coordination 8:8.

    • module-2
    • ionic
    Calorimetry

    Measuring heat, by watching how much a known amount of material warms or cools.

    • module-7
    • calorimetry
    Canonical ensemble

    An imaginary pile of many copies of the whole system, all with the same number of particles, volume and temperature.

    • module-6
    • statistical mechanics
    Canonical partition functionQ

    The sum of exp(-E/kT) over every state of the whole system. It replaces the molecular partition function when particles interact.

    • module-6
    • statistical mechanics
    Carrier concentrationn

    The number of charge carriers per volume that can be excited to move. Only electrons within a few kT of the Fermi level count.

    • module-3
    • transport
    Carrier mobilitymu

    How easily carriers move, mu = e tau / m*. Impurities and lattice vibrations lower it.

    • module-3
    • transport
    Catalyst

    Something that speeds up a reaction by lowering the Gibbs free energy of activation. It does not change where the reaction ends up.

    • module-9
    • kinetics
    Characteristic temperatureΘ = ΔE/k

    The temperature set by a system energy spacing. Well above it the system is hot and many states are used. Well below it only the ground state is used.

    • statistical mechanics
    Chemical potentialμ

    What becomes equal between a system and its surroundings when particles can swap across the boundary.

    • thermodynamics
    Chiral

    A molecule that cannot be put on top of its mirror image, like a left and right hand. It has no improper symmetry element.

    • module-1
    • symmetry
    Cholesteric phasechiral nematic

    A nematic made of twisted-handed molecules, where the pointing direction turns slowly along an axis. The distance for one full turn is the pitch.

    • module-8
    • liquid crystals
    Classical mechanics

    Describes the world with positions and velocities (trajectories). Fine when the de Broglie wavelength is much smaller than the system.

    • module-1
    • models
    Clausius-Clapeyron equation

    The slope of a phase boundary on a pT diagram: dp/dT equals the entropy change divided by the volume change of the transition.

    • module-6
    • thermodynamics
    Coercive fieldE_c (electric), H_c (magnetic)

    The reverse field needed to bring the net polarisation (or magnetisation) back to zero.

    • module-3
    • dielectrics
    • magnetism
    Coexistence

    Two phases, such as liquid and gas, present together at equilibrium, with the same chemical potential.

    • module-6
    • phase transitions
    Colloid

    A mixture where tiny particles stay spread through a liquid. The particles are between the size of a solution and a suspension.

    • module-8
    • soft matter
    Conduction band

    The band made of unoccupied orbitals. Electrons promoted into it can carry current.

    • module-3
    • band theory
    Conductivitysigma

    How well a material carries current, in S per cm. It is the inverse of resistivity, sigma = 1/rho.

    • module-3
    • transport
    Configuration (macrostate)

    A group of microstates that give the same bulk property, like "two heads out of four coins". In chemistry it is the list of occupation numbers.

    • statistical mechanics
    Cooper pair

    Two electrons paired up at low temperature (BCS theory). The pairs move through the lattice without scattering, which gives zero resistance.

    • module-3
    • superconductivity
    Coordination number

    How many nearest neighbours an atom or ion has. For ionic crystals it is written cation first, then anion.

    • module-2
    • ionic
    Critical point

    The end of the liquid-gas line on a phase diagram. Beyond it liquid and gas cannot be told apart.

    • module-6
    • phase transitions
    Critical radiusr*

    The size a nucleus must reach to survive. Smaller ones shrink, bigger ones grow. r* = 2 gamma / DeltaG_V.

    • module-7
    • kinetics
    Critical temperatureT_c

    The temperature below which a material becomes superconducting.

    • module-3
    • superconductivity
    Crystal system

    One of seven cell shapes: triclinic, monoclinic, orthorhombic, tetragonal, trigonal, hexagonal, cubic.

    • module-2
    • crystals
    Cubic close-packed (ccp, fcc)

    Spheres stacked in layers ABCABC. The same as face-centred cubic. 12 nearest neighbours and 74 percent of space filled.

    • module-2
    • packing
    Curie law

    The paramagnetic susceptibility falls with temperature as chi = C_Curie / T.

    • module-3
    • magnetism
    Curie temperatureT_C

    The temperature at which a ferroelectric becomes paraelectric, or a ferromagnet becomes paramagnetic. For BaTiO3 it is 120 C.

    • module-3
    • dielectrics
    • magnetism
    Curie-Weiss law

    The susceptibility above the ordering temperature of a ferromagnet or antiferromagnet, chi = C/(T - theta).

    • module-3
    • magnetism
    de Broglie wavelengthlambda = h / p

    The size of the wave that goes with a moving particle. If it is much smaller than the thing you study, you can treat the particle classically.

    • module-1
    • models
    Debye temperaturehbar omega / k_B

    A temperature standing for the collective (acoustic) vibration of the lattice. It appears in the BCS equation.

    • module-3
    • superconductivity
    Defect

    A flaw in an otherwise perfect crystal, like a missing egg in an egg tray. Defects change strength, conductivity and colour.

    • module-6
    • defects
    Degeneracyg

    The number of states that share one energy level.

    • statistical mechanics
    Delocalised electronic conduction

    Conduction by electrons spread over the whole crystal through a band, as in metals, silicon and graphite. The opposite is localised conduction.

    • module-3
    • conduction
    Dendrite

    A branching, tree-like crystal that grows when diffusion limits growth and the tips get the most supply, as in a snowflake.

    • module-7
    • kinetics
    Density of statesDOS

    The number of permitted electronic states in an energy interval. In plain words, how many seats there are at each energy.

    • module-3
    • band theory
    Diamagnetism

    A weak repulsion from a magnetic field that all materials show, from paired electrons. chi is negative and temperature-independent.

    • module-3
    • magnetism
    Dielectric

    An electrical insulator that can be polarised by an applied electric field. Its charges shift slightly when a field is applied.

    • module-3
    • dielectrics
    Differential rate law

    An equation for how fast a concentration is changing right now, in terms of the concentrations.

    • module-9
    • kinetics
    Diffusion

    Net movement of matter from high to low concentration, caused by random motion of the particles.

    • module-8
    • diffusion
    Diffusion-controlled reaction

    A reaction that happens every time the partners touch. Its speed is set only by how fast and how far the partners diffuse.

    • module-9
    • kinetics
    Dimensional analysis

    A quick estimate that uses how quantities scale with size, for example mass with length cubed and area with length squared, to test an idea.

    • module-1
    • models
    Director

    The average direction that the rods point in a liquid crystal. Written as n-bar.

    • module-8
    • liquid crystals
    Dislocation

    A line defect. Edge dislocations are an extra half-row of atoms. Screw dislocations spiral like a staircase.

    • module-6
    • defects
    Double exchange

    An unpaired electron hopping between magnetic ions of different oxidation states, easy only if spins stay aligned. It favours ferromagnetic order.

    • module-3
    • magnetism
    Drude model

    The conductivity formula sigma = n e^2 tau / m*, built from carrier number, charge, relaxation time and effective mass.

    • module-3
    • transport
    DSCdifferential scanning calorimetry

    A technique that heats a sample and an empty reference pan at the same rate and records the extra heater power the sample needs. Works on milligram samples.

    • module-7
    • calorimetry
    Dulong-Petit law3R = 24.9 J/K/mol

    At high temperature the molar heat capacity of a simple solid approaches 3R.

    • thermodynamics
    Effective ionic radius

    The size given to an ion, based on the minimum in electron density between ions. It depends on coordination number.

    • module-2
    • ionic
    Effective massm*

    How heavy a carrier acts in a crystal. It depends on band width, which depends on orbital overlap.

    • module-3
    • transport
    Ehrenfest classification

    Sorting phase transitions by which derivative of the Gibbs energy is discontinuous.

    • module-7
    • phase transitions
    Einstein solid

    A model where each atom of a crystal is an independent 3D harmonic oscillator, and all share one frequency.

    • statistical mechanics
    Electric susceptibilitychi_e

    The size of the polarisation response, chi_e = epsilon_r - 1, with P = epsilon_0 chi_e E.

    • module-3
    • dielectrics
    Electron density map

    A 3D map of where the electrons are, built from the diffraction pattern. It shows geometry and bonding.

    • module-2
    • diffraction
    Elementary process

    A single real step in a reaction, either one molecule changing or two molecules meeting. Its rate law follows from its molecularity.

    • module-9
    • kinetics
    EnthalpyH = U + pV

    Internal energy plus pV. At constant pressure, its change equals the heat flowing in. Exothermic and endothermic usually refer to its change.

    • thermodynamics
    EntropyS = k ln W

    A measure of how many microstates a configuration has. More ways to arrange things means higher entropy.

    • thermodynamics
    • statistical mechanics
    Excluded volumeNb

    The room the molecules themselves take up, which is not free for them to move in.

    • module-6
    • phase transitions
    Expectation value

    An average over states, with each state weighted by how likely it is.

    • statistical mechanics
    Extrinsic defect

    A defect that thermodynamics does not require, such as an impurity atom.

    • module-6
    • defects
    Extrinsic semiconductor

    A semiconductor with a deliberate impurity added (doped). Most semiconductors used in electronics are this kind.

    • module-3
    • semiconductors
    Fermi levelE_F

    A hypothetical electron energy at which the probability of occupation is 50%. In a metal it sits inside a partly filled band.

    • module-3
    • band theory
    Ferrimagnetism

    Opposing moments that do not cancel, so there is a spontaneous net magnetisation. Magnetite is an example.

    • module-3
    • magnetism
    Ferroelectric

    A dielectric with spontaneous polarisation that is kept when the field is removed.

    • module-3
    • dielectrics
    Ferromagnetism

    All spins aligned, giving spontaneous magnetisation below the Curie temperature.

    • module-3
    • magnetism
    Fick's first law

    The flux across a surface is proportional to the area and to the concentration gradient. J = -D A dc/dx.

    • module-8
    • diffusion
    Fick's second law

    How the concentration at a point changes with time. dc/dt = D d2c/dx2. Bumps flatten and dips fill.

    • module-8
    • diffusion
    First law of thermodynamics

    Energy is conserved. In this unit, the change in internal energy equals heat entering plus work done on the system: delta U = Q + W.

    • thermodynamics
    First-order transition

    A transition with latent heat, where the first derivatives of G (entropy and volume) jump. Boiling and freezing are examples.

    • module-7
    • phase transitions
    Fractional coordinates

    Where an atom sits in the cell as fractions (0 to 1) of each cell edge.

    • module-2
    • crystals
    Frenkel defect

    An atom that has hopped out of its site into a nearby gap, leaving a vacancy behind. Found where ion sizes differ a lot, like AgCl.

    • module-6
    • defects
    Fundamental postulate

    Every microstate is equally likely. So the most likely configuration is the one with the most microstates.

    • statistical mechanics
    Gibbs free energyG = H - TS

    The test for spontaneous change at constant temperature and pressure. A spontaneous change has delta G of zero or less.

    • thermodynamics
    Glass

    An amorphous solid that shows a glass transition. Think of a liquid frozen in place before it could crystallise.

    • module-7
    • glasses
    Glass transitionT_g

    The gradual, reversible change between the brittle glass and the liquid on heating. It happens over a range that depends on cooling rate.

    • module-7
    • glasses
    Glide plane

    A reflection followed by a slide, usually half a cell edge or diagonal. It changes handedness.

    • module-2
    • crystals
    Grain boundary

    The surface between two crystal grains that point in different directions in a polycrystalline solid.

    • module-6
    • defects
    Half-life

    The time for a concentration to fall to half. For first order it is ln(2)/k and does not depend on the starting concentration.

    • module-9
    • kinetics
    Hard-particle model

    A model where particles cannot overlap and have no other forces. With no interaction energy, only entropy decides the stable phase.

    • module-8
    • liquid crystals
    HeatQ

    Energy that crosses the boundary because of a temperature difference. It is energy in motion, not energy stored.

    • thermodynamics
    Heat capacityC = dQ/dT

    How much heat you must add to raise the temperature by one unit.

    • thermodynamics
    Helmholtz free energyA = U - TS

    The most work you can get out of a system at constant temperature. At constant T and V a spontaneous change lowers A.

    • thermodynamics
    Heterogeneous nucleation

    Seeds of the new phase starting on a wall or an impurity particle.

    • module-7
    • kinetics
    Hexagonal close-packed (hcp)

    Spheres stacked in layers ABAB. Each sphere has 12 nearest neighbours.

    • module-2
    • packing
    Homogeneous nucleation

    Seeds of the new phase appearing spontaneously inside the liquid itself.

    • module-7
    • kinetics
    Identity (E)

    The operation that does nothing. Every molecule has it.

    • module-1
    • symmetry
    Importance sampling

    Generating configurations with the probability they have at equilibrium, so each can be counted equally, instead of weighting random ones afterwards.

    • module-6
    • simulation
    Improper operation

    Any operation with a reflection or inversion in it. It flips handedness. A molecule with one cannot be chiral.

    • module-1
    • symmetry
    Improper rotation (Sn)

    A rotation by 360/n followed by a reflection in the plane across the axis. S1 is the same as sigma and S2 is the same as i.

    • module-1
    • symmetry
    Inert pair effect

    Heavy cations such as Sn2+, Pb2+ and Bi3+ keep a lone pair of s electrons that is not spherical, which distorts the structure.

    • module-3
    • dielectrics
    Integrated rate law

    An equation for the concentration at any time. It is what you get by integrating the differential rate law.

    • module-9
    • kinetics
    Intercalation

    Sliding atoms or molecules between the layers or cages of a host, such as K into graphite to give KC8, or alkali metals into C60.

    • module-3
    • conduction
    Interfacial energygamma

    The energy cost of creating a surface between the new and old phase. Always positive.

    • module-7
    • kinetics
    Internal energyU

    The total energy of all the molecules in their occupied states.

    • thermodynamics
    Interstitial impurity

    A foreign atom squeezed into a hole between the regular atoms. Hydrogen in palladium is an example.

    • module-6
    • defects
    Intrinsic defect

    A defect that thermodynamics makes, such as a Schottky or Frenkel pair. All solids have some above absolute zero.

    • module-6
    • defects
    Intrinsic semiconductor

    A pure, undoped semiconductor. Heating promotes electrons from the valence band to the conduction band across a small gap.

    • module-3
    • semiconductors
    Inversion axis (n-bar)

    A rotation by 360/n followed by inversion through a centre point. Used mostly for crystals.

    • module-1
    • symmetry
    Inversion centre (i)

    A point through which every atom can be sent straight across to an identical atom at the same distance on the other side.

    • module-1
    • symmetry
    Ionic conductivity

    Electric current carried by ions hopping through a solid, which needs defects to move through.

    • module-6
    • defects
    Ising model

    A lattice of spins that can only point up or down, interacting with nearest neighbours. The simplest model of a magnet.

    • module-6
    • magnetism
    Isochoric and isobaric

    Isochoric means constant volume. Isobaric means constant pressure.

    • thermodynamics
    Isoelectronic

    Having the same number of valence electrons. In the lecture, elements in the same group.

    • module-1
    • bonding
    Ketelaar's triangle

    A triangle showing a smooth range between ionic, covalent and metallic bonding.

    • module-2
    • ionic
    Krogmann salt

    Partly oxidised K2[Pt(CN)4], the first molecular metal. It conducts along chains of platinum units (1D).

    • module-3
    • conduction
    kTBoltzmann constant times temperature

    The size of a typical thermal push. About 2.5 kJ/mol at 25 degrees C. An energy gap much bigger than kT is almost never crossed by heat alone.

    • module-8
    • soft matter
    Latent heat

    Heat absorbed or released during a change of state without the temperature changing, like ice melting in a drink.

    • module-7
    • calorimetry
    Lattice enthalpyDelta H_L

    The energy to pull one mole of an ionic crystal apart into separate gaseous ions.

    • module-2
    • ionic
    Lyotropic phase

    An ordered phase that forms when molecules such as amphiphiles are dissolved. The phase depends on concentration and temperature, and can shift with pH or salt.

    • module-8
    • liquid crystals
    Madelung constantA

    A number that depends on the crystal structure. It adds up the attraction and repulsion from every shell of neighbours around an ion.

    • module-2
    • ionic
    Magnetic domain

    A patch of a magnet where all the spins line up. If the domains point randomly, the piece has no net magnetisation.

    • module-6
    • magnetism
    Magnetic susceptibilitychi

    How strongly a material becomes magnetised in a field, from M = chi H. Negative for diamagnets, positive for the others.

    • module-3
    • magnetism
    MagnetisationM

    Magnetic moment per unit volume of a material.

    • module-3
    • magnetism
    MagnetiteFe3O4, lodestone

    A ferrite with an inverse spinel structure. It is ferrimagnetic and conducts through Fe2+ <-> Fe3+ + e-.

    • module-3
    • magnetism
    Martensite

    A very hard metastable form of steel made by quenching, which is why quench hardening works.

    • module-7
    • glasses
    Mean-field theory

    An approximation that replaces all the separate pushes and pulls a particle feels with one average push. It is crude but shows transitions clearly.

    • module-6
    • phase transitions
    Meissner effect

    A superconductor pushing magnetic fields out of itself as it cools through its critical temperature. It is perfect diamagnetism.

    • module-3
    • superconductivity
    Mesogen

    A molecule that can form a mesophase.

    • module-8
    • liquid crystals
    Mesophase

    An equilibrium phase between liquid and crystal. It has some liquid properties, such as flowing, and some crystal properties, such as long-range alignment.

    • module-8
    • liquid crystals
    Metastable

    Not at equilibrium but stuck in a shallow dip behind an energy barrier, like a book standing on its edge. Glass, diamond and martensite are examples.

    • module-7
    • glasses
    Metropolis rule

    Accept a move that lowers the energy. Accept one that raises it with probability exp(-beta dE).

    • module-6
    • simulation
    Microstate

    One exact arrangement of every individual molecule, like which coin is heads and which is tails.

    • statistical mechanics
    Miller indices (h k l)

    Three whole numbers that name a plane in a crystal. The plane cuts the axes at 1/h, 1/k and 1/l. A negative index has an overbar.

    • module-2
    • diffraction
    Mirror plane (sigma)

    An imaginary plane where one side is the mirror image of the other. sigma_v contains the principal axis. sigma_h is perpendicular to it.

    • module-1
    • symmetry
    Model

    A simplified picture of part of the natural world. It is simple enough to understand and still captures something real. A map is a model.

    • module-1
    • models
    Molar heat capacity

    Heat capacity per mole of substance.

    • module-7
    • calorimetry
    Molecular dynamicsMD

    A simulation that follows atoms through time by solving Newton's laws step by step.

    • module-6
    • simulation
    Monte Carlo simulation

    A method that makes random trial moves and accepts or rejects them by a rule, to sample equilibrium configurations. It gives no real time dynamics.

    • module-6
    • simulation
    Mott-Hubbard insulator

    A material where atoms are far enough apart that the band model fails and electrons stay on individual atoms or molecules, so it does not conduct.

    • module-3
    • conduction
    n-type semiconductor

    A doped semiconductor whose carriers are negative electrons. The dopant has occupied levels just below an empty conduction band, such as As in Si.

    • module-3
    • semiconductors
    Neel temperatureT_N

    The temperature below which an antiferromagnet orders. For an antiferromagnet theta = -T_N.

    • module-3
    • magnetism
    Nematic phase

    A mesophase where rod-shaped molecules point the same way on average but are not arranged in layers or at fixed sites.

    • module-8
    • liquid crystals
    Nucleation

    The first appearance of tiny seeds of a new phase inside the old one.

    • module-7
    • kinetics
    Nucleation barrierDeltaG*

    The energy hump a nucleus has to climb to reach the critical radius. It falls with deeper undercooling.

    • module-7
    • kinetics
    Occupation numbern_i

    How many molecules are in quantum state i.

    • statistical mechanics
    Octahedral hole

    The gap among six packed spheres. There is one per ccp atom, with size ratio 0.414.

    • module-2
    • packing
    Onsager theory

    A calculation that predicts, from rod shape alone, the concentrations where the isotropic and nematic phases are stable. It balances orientational entropy against translational entropy.

    • module-8
    • liquid crystals
    Open, closed and isolated system

    Open swaps matter and energy with the outside. Closed swaps energy only. Isolated swaps neither.

    • thermodynamics
    Order parameterS

    One number that says how well rods line up. It is 1 for perfect alignment and 0 for a random (isotropic) crowd.

    • module-8
    • liquid crystals
    Ostwald ripening

    Small particles dissolve while large ones grow, so the structure coarsens over time.

    • module-7
    • kinetics
    p-n junction

    An n-type and a p-type semiconductor joined together. Electrons diffuse from n to p and set up an electric field. It lets current pass one way, and a solar cell is one.

    • module-3
    • semiconductors
    p-type semiconductor

    A doped semiconductor whose carriers are positive holes. The dopant has empty levels just above a full valence band, such as Ga in Si.

    • module-3
    • semiconductors
    Paraelectric

    A dielectric that polarises when a field is applied and loses the polarisation when the field is removed.

    • module-3
    • dielectrics
    Paramagnetism

    Attraction to a field from unpaired electrons that the field aligns. chi is positive and follows Curie law, chi = C/T.

    • module-3
    • magnetism
    Partition functionq

    The sum of e to the minus beta epsilon over all states. Roughly the number of states a molecule can reach at this temperature.

    • statistical mechanics
    Pauli exclusion principle

    No two electrons in an atom can have all four quantum numbers the same. An orbital holds at most two electrons.

    • module-1
    • bonding
    Periodic boundary conditions

    Surrounding a small simulation box with copies of itself so that a particle leaving one side comes back in the other.

    • module-6
    • simulation
    Perovskite

    A structure with the formula ABX3, where A is a 12-coordinate cation, B an octahedral cation and X an anion. BaTiO3 is an example.

    • module-3
    • dielectrics
    Phase

    A state of matter whose properties change smoothly, such as ice, liquid water or water vapour.

    • module-6
    • phase transitions
    Phase diagram

    A map of pressure and temperature (or volume) showing which phase is stable where, with boundary lines where two phases coexist.

    • module-6
    • phase transitions
    Phase transition

    An abrupt change in a physical property, like the jump in density when water boils. It needs interactions between particles.

    • module-6
    • phase transitions
    Photovoltaic diodePV diode, solar cell

    A p-n junction where incoming photons keep supplying new electrons and holes, so a current flows.

    • module-3
    • semiconductors
    Piezoelectric effect

    Stress on a material produces a voltage. The reverse effect is a voltage changing the material size.

    • module-3
    • dielectrics
    Pitch

    In a cholesteric, the distance over which the director rotates a full turn.

    • module-8
    • liquid crystals
    Point defect

    A flaw at a single lattice site, or a few. It is zero-dimensional. Vacancies, interstitials and impurities are examples.

    • module-6
    • defects
    Point group

    The full set of symmetry operations of a molecule. Molecules with the same symmetry share a point group.

    • module-1
    • symmetry
    PolarisationP

    The shift of charges in a dielectric under a field. The lecture lists electronic, ionic, orientation and space charge mechanisms.

    • module-3
    • dielectrics
    Polarised light

    Light whose electric field shakes in one direction only.

    • module-8
    • optics
    Potential energy curve

    A graph of energy against the distance between two atoms. It dips to a minimum where the bond sits and rises steeply when the nuclei get too close.

    • module-1
    • bonding
    Potential energy surface

    A landscape of energy against the positions of the atoms. Reactants sit in one valley, products in another.

    • module-9
    • kinetics
    Pre-equilibrium

    A fast reversible step that stays in equilibrium while one of its products slowly goes on to react in a later step.

    • module-9
    • kinetics
    Principal axis

    The rotation axis with the highest n. By convention it is the z-axis.

    • module-1
    • symmetry
    Principle of detailed balance

    At equilibrium, the forward and backward rates of every elementary step are equal.

    • module-9
    • kinetics
    Proper operation

    The identity or a pure rotation. It keeps handedness.

    • module-1
    • symmetry
    Quantum mechanics

    Describes the world with wave functions. Needed for light particles such as electrons and for very low temperatures.

    • module-1
    • models
    Radius ratior cation / r anion

    The size of the cation divided by the size of the anion. A bigger ratio gives a higher coordination number.

    • module-2
    • ionic
    Random walk

    A path made of steps in random directions. It models Brownian motion. One walker is unpredictable, but the average of x squared across many walkers grows linearly with time.

    • module-8
    • diffusion
    Rate-determining step

    The slowest step in a mechanism, which acts as the bottleneck for the overall rate.

    • module-9
    • kinetics
    Reaction mechanism

    The list of elementary steps that make up an overall reaction. The rate law comes from the mechanism, not from the balanced equation.

    • module-9
    • kinetics
    Reciprocal lattice

    The lattice whose points are the diffraction spots. A pattern is a slice through it.

    • module-2
    • diffraction
    Recurrent and transient random walks

    A recurrent walk keeps coming back to its start. A transient walk may never return. 2-d walks are recurrent and 3-d walks are transient.

    • module-8
    • diffusion
    Relative permittivitydielectric constant, epsilon_r

    How readily a material polarises in a field, compared with vacuum (which is 1). It has no units. Inserting the material multiplies a capacitor capacitance by this factor.

    • module-3
    • dielectrics
    Relaxation timetau

    The average time a carrier travels between scattering events.

    • module-3
    • transport
    Remnant polarisationP_r

    The polarisation left when the field returns to zero after a strong field.

    • module-3
    • dielectrics
    Reservoir

    Surroundings so big that taking or giving some heat does not change their temperature.

    • thermodynamics
    Residual entropy

    Entropy left over at absolute zero because the lowest-energy arrangement is not unique. CO, ice and spin ice are examples.

    • thermodynamics
    Reversible process

    A process that is always at equilibrium, so it runs infinitely slowly.

    • thermodynamics
    Rock-salt structure

    NaCl type. ccp anions with all octahedral holes filled by cations. Coordination 6:6.

    • module-2
    • ionic
    Rotation axis (Cn)Rotation by 360 degrees / n

    A line you can turn the molecule about, by 360/n degrees, so it looks the same.

    • module-1
    • symmetry
    Rutile

    TiO2 type. Distorted hcp anions with half the octahedral holes filled. Coordination 6:3.

    • module-2
    • ionic
    Saturation polarisationP_s

    The polarisation reached in a strong field when all domains are aligned.

    • module-3
    • dielectrics
    Schoenflies notation

    The point group naming that chemists use for molecules, such as C3v and D6h.

    • module-1
    • symmetry
    Schottky defect

    A pair of empty sites, one where a cation should be and one where an anion should be. Found in crystals like NaCl with highly coordinated ions of similar size.

    • module-6
    • defects
    Screw axism_n

    A turn plus a slide, like a spiral staircase. m_n means slide n/m of the cell and turn 360/m degrees. It keeps handedness.

    • module-2
    • crystals
    Second harmonic generationSHG

    Two photons combine into one with twice the energy, such as red light turned into green in a KTP laser. The crystal has no inversion centre.

    • module-3
    • dielectrics
    Second law of thermodynamics

    The entropy of an isolated system always increases. Heat flows from hot to cold by itself.

    • thermodynamics
    Second-order transition

    A transition with no latent heat, where entropy and volume are continuous and the second derivative of G jumps. Ferromagnetic and superconducting transitions are examples.

    • module-7
    • phase transitions
    Selective reflection

    A cholesteric bounces back some colours of white light and lets the rest through, because of its repeating twist.

    • module-8
    • optics
    Self-consistency equation

    An equation with the unknown on both sides, such as m/N = tanh(beta J d m/N), solved by finding where two curves cross.

    • module-6
    • magnetism
    Semi-metal

    A material like graphite where thermal energy promotes a small number of electrons into the conduction band.

    • module-3
    • conduction
    Smectic phase

    A mesophase where the rods point the same way and also sit in layers.

    • module-8
    • liquid crystals
    Soft matter

    Anything that can be changed by pushes as small as the random jostling of heat. Polymers, colloids and liquid crystals are examples.

    • module-8
    • soft matter
    Space group

    A point group combined with translation. There are 230 of them. It lists every symmetry element of a crystal.

    • module-2
    • crystals
    Specific heat capacity

    Heat capacity per unit mass (the slides say per gram). It lets you compare materials fairly.

    • module-7
    • calorimetry
    Spinodal decomposition

    Phase separation of a mixture with no nucleation barrier, driven only by diffusion. The whole mixture clumps into two phases.

    • module-7
    • kinetics
    Stacking fault

    A planar defect where the usual sequence of close-packed layers (ABC for fcc, ABA for hcp) breaks.

    • module-6
    • defects
    State function

    A quantity that depends only on the current state of the system, not on how it got there.

    • thermodynamics
    Steady state approximation

    The assumption that a short-lived intermediate quickly reaches a constant concentration, so its rate of change is zero.

    • module-9
    • kinetics
    Stirling approximation

    A shortcut for the log of a huge factorial: ln n! is about n ln n minus n.

    • statistical mechanics
    Substitutional impurity

    A foreign atom sitting on a normal lattice site, taking the place of a regular atom. Chromium in ruby is an example.

    • module-6
    • defects
    Superconductor

    A material that below its critical temperature has zero resistivity and completely expels magnetic fields.

    • module-3
    • superconductivity
    Supercooled liquid

    A liquid cooled below its melting point that has not crystallised. A glass is a deeply supercooled liquid.

    • module-7
    • glasses
    Supercritical fluid

    The single fluid phase above the critical point. Supercritical CO2 is used as a solvent, for example to decaffeinate coffee.

    • module-6
    • phase transitions
    Superexchange

    Indirect magnetic exchange between non-neighbouring magnetic atoms through a non-magnetic atom between them. It favours antiferromagnetic order.

    • module-3
    • magnetism
    Symmetry element

    The axis, plane or point that a symmetry operation is carried out about.

    • module-1
    • symmetry
    Symmetry operation

    A move that takes a molecule onto itself, so atoms land on equivalent atoms.

    • module-1
    • symmetry
    Tetrahedral hole

    The gap among four packed spheres. There are two per ccp atom. Lecture 7 gives size ratio 0.225 and Lecture 5 gives 0.255.

    • module-2
    • packing
    Thermal wavelengthΛ

    A length built from h, m and beta. The translational partition function is the volume divided by Lambda cubed.

    • statistical mechanics
    Thermodynamic limit

    What you get when the number of molecules grows without end. Only the most likely configuration is ever seen.

    • statistical mechanics
    Third law of thermodynamics

    The entropy of a system approaches a constant value as the temperature goes to zero. For a perfect crystal that value is zero.

    • thermodynamics
    Tight-binding approximation

    The picture where atomic orbitals overlap with their neighbours. More atoms means more molecular orbitals, and in a crystal they merge into bands.

    • module-3
    • band theory
    Transition state

    The configuration at the top of the pass between reactant and product valleys. It is the saddle point of the potential energy surface.

    • module-9
    • kinetics
    Transition state theoryTST

    A way to get a rate coefficient by treating the reactants and transition state as in equilibrium and multiplying by the rate of leaving the transition state.

    • module-9
    • kinetics
    Translational symmetry

    Shift the whole crystal by a unit cell edge and it looks the same.

    • module-2
    • crystals
    Triple point

    The one temperature and pressure where solid, liquid and gas coexist. For water it is 0.01 degrees C and 612 Pa.

    • module-6
    • phase transitions
    TTF-TCNQ

    The first organic metal. Donor TTF gives charge to acceptor TCNQ and the stacks conduct along one direction.

    • module-3
    • conduction
    Tungsten bronze

    Na-doped WO3, NaxWO3, where the sodium donates x electrons per tungsten into the conduction band and makes the oxide metallic.

    • module-3
    • conduction
    Undercoolingsupercooling, DeltaT

    Cooling a liquid below its melting point without it freezing. The amount is DeltaT = T_m minus the actual temperature.

    • module-7
    • kinetics
    Unit cell

    The smallest box that, copied along the cell vectors, builds the whole crystal.

    • module-2
    • crystals
    Valence band

    The band made of occupied orbitals. In plain words, the full car park.

    • module-3
    • band theory
    Valence electrons

    The outer electrons that take part in bonding.

    • module-1
    • bonding
    van der Waals equation

    The ideal gas law with two fixes: take away the volume of the molecules, and lower the pressure for their mutual attraction.

    • module-6
    • phase transitions
    Viscosity

    How thick a fluid is, its resistance to flow. Water is about 10^-4 Pa s, ketchup 10 Pa s, pitch about 10^8 Pa s.

    • module-7
    • glasses
    VSEPRValence shell electron pair repulsion

    Electron groups around an atom push each other as far apart as they can. That fixes the molecule shape.

    • module-1
    • bonding
    Weight of a configurationW

    How many microstates make up one configuration. W = N! divided by n0! n1! n2! and so on.

    • statistical mechanics
    WorkW

    Energy moved by a force pushing something through a distance. In a gas, work is the push on a piston.

    • thermodynamics
    YSZyttria-stabilised zirconia

    A zirconia ceramic doped with yttrium so it carries oxide ions. It is the electrolyte in the solid-oxide fuel cell.

    • module-6
    • defects
    Zeroth law of thermodynamics

    If two things are each in thermal equilibrium with a third, they are in equilibrium with each other. This is why a thermometer works.

    • thermodynamics
    Zinc blende (sphalerite)

    ZnS type. ccp anions with half the tetrahedral holes filled. Coordination 4:4.

    • module-2
    • ionic