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119 Cards in this Set

  • Front
  • Back

conversion between eV and cm-1

1eV = 8066cm-1

gross structure

electron and nuclear attraction


electron electron repulsion


electron kinetic energy

fine structure

spin orbit interactions


relativistic corrections

hyperfine structure

nuclear attractions

wavenumber

1/wavelength

reduced mass

1/m = 1/me + 1/mn

energy using rydbergs constant

En = - Rh/n^2 =

R infinity hc

equations for the transition between states

equations for bohr radius and fine structure constant

angular momentum operator

probability in terms of radial function

P(r) =r^2R(r)^2

eigenfunction of L^2 operator

values of ml

normalisation

electric dipole

2 oppositely charged charges separated by a distance



vibrations of electrons. create fluctuating dipole

spontaneous emissions

emission of a photon when an atom de-excites

homogenous broadening

affects all indivual atoms in the same way



natural and collision broadening

inhomogeneous broadening

affects atoms in different ways



found in solids where atoms experience different local environments

assumption for atoms

that they are spherical symmetric

equation for electric dipole

p=qd

fermi's golden rule

W12 = (2pi/hbar)|M12|^2 g(hf)

equation for parity

parity = (-1)^L

Einstein constant A

A=1/tau

equation for the time between collisions

observable frequency for doppler broadening

f = f0(1±vx/c)

non radiative transition time

1/tau = A + 1/tau(non radiative)

polarised light in terms.of perturbation

collision broadening

gas collides with the wall and interrupts the emission of light



uncertainty principle

selection rules

natural broadening

photon emitted causes a burst of light that decays exponentially



caused lorentzian line



delta E delta t > h bar

doppler broadening

thermal motion



doppler shift in frequency

aufbau principle

the filling up of shells in order of increasing every

quantum defect

allows for perturbation of inner shells by the valence electrons

bohr formula

z can be z effective

types of series

k series n=1e has been ejected


l series n=2e


m series n=3e

shell model

evidence for Shell model

absorption edge

equation for quantum defect

screening

emission spectra

spin orbit coupling

force on a magnetic dipole

Fz = uz (dB/dz)

spin momentum

spin orbit interaction and types of coupling based on interaction

what happens to L+S when there are 2 electrons

has to be even

evidence for spin

LS coupling

shorthand

rules for ground state (hunds rules)

helium wavefunction

Pauli exclusion principle

absense of a triplet is the same as trying to put 2e- in same state

exchange energy

gyrometric ratio (gamma)

e/2m



it specifies the proportionally constant between angular momentum and its magnetic moment

Thomas precession

reduces energy by a factor of 2

interval rule

levels with same L and S but different J are separated by an energy that is proportional to J

mass effects

changes in nuclear mass make changes to reduced mass hence energies

field effects

electrons in s shell have a finite probability of penetrating the nucleus therefore sensitive to charge distribution

comparison of nucleus to electrons

total momentum including nuclear momentum

magnetic moment and derivation

magnetic moment z component

magnetic field in z

Bz = u0I/2r

Central field

spin on nucleus

hyperfine energy

<I. J>

normal zeeman effect

longitudinal observation of normal. zeeman effect

transverse observation of normal zeeman effect

quantum confined stark effect

exciton from optical absorption


binding energy is small


very unstable

pashen back effect

anomalous zeeman effect

quadratic stark effect

small redshift is proportional to root energy

linear stark effect

definition of laser

an oscillator as well as an amplifier



amplification achieved by stimulated emission

losses from a laser

positive feedback diagram

condition for oscillation

A and B coefficients of emission and absorption

population inversion

four level system

three level system

define cavity

provided positive feedback that turns an amplifier into an oscillator

define transverse modes

describe the variation if the E field across a cross section of a beam.

define longitudinal modes

determines emission spectra

multimode operation

for a given longitudinal mode to oscillate, its frequency must lie within the emission spectra

single mode operation

make laser with one mode

mode locking

emission of a continuous train of short pulses

active technique

time independent shutter opened every 2L/c seconds

passive technique

saturable absorber put into cavity

spatial coherence

related to phase uniformity across a cross section



high in single modes

temporal coherence

refers to time duration over which the phase is constant

H n and m values

Length of cavity

L = int x c/2nf

frequency in cavity

f = int x c/2nl

minimum pulse duration

delta t min delta f > 1/2pi

temporal coherence time

tc = 1/detla f

coherence length

lc = ct = c/delta f

root mean squared velocity

v = root(3kt/m)

doppler shifted frequency

max force on an atom

Fx = - h/lamda tau

deceleration

ax = - h/mlamda tau

cycles to stop an atom

N =mu(x) lamda/h

min time to stop an atom

tmin = N(stop) x tau

min distance travelled to stop an atom

d = u(x) ^2/2a^2

doppler limit temperature

T = h bar /2Kb tau

recoil temperature

T = h^2/mKlamda^2

debroglie wavelength

lamda = h/root(3mkT)

wavefunction overlap

N/V = 1/debroglie wavelength ^2

temperature of condensation

Tc = 1/3 h^2/mk (N/V) ^2/3

BEC

optical molasses

fix laser beam arrangement to. stop atoms moving in all 3 directions

magneto-optical trap

add magnetic coils above and below laser beams

low field seeking

experience potential minimum at the centre


traps then close to origin

sisphysis cooling

atoms repeatedly climb to top. of. potential created by stark effect and then drop down after absorption and emission of a photon

procedure of BEC

what does doppler cooling ignore

stimulated emission

temp comparison between optical molasses and doppler limit

optical molasses cools atoms to below temp of doppler limit.