-
1
-
-
0001482180
-
Magnetic optical activity
-
ARPLAP, 0066-426X, 10.1146/annurev.pc.17.100166.002151, See, for example, references therein.
-
Buckingham AD, Stephens PJ. Magnetic optical activity. Annu. Rev. Phys. Chem. 1966, 17:399-432. ARPLAP, 0066-426X, 10.1146/annurev.pc.17.100166.002151, See, for example, references therein.
-
(1966)
Annu. Rev. Phys. Chem.
, vol.17
, pp. 399-432
-
-
Buckingham, A.D.1
Stephens, P.J.2
-
2
-
-
0003898668
-
-
radiation induced m=1 transitions on absorption (m is the magnetic quantum number).
-
radiation induced m=1 transitions on absorption (m is the magnetic quantum number).
-
(1964)
Optics
, pp. 101-106
-
-
Sommerfeld, A.1
-
3
-
-
0011602553
-
Faraday rotation in the undergraduate advanced laboratory
-
AJPIAS, 0002-9505, 10.1119/1.13164, AJPIAS, 0002-9505, 10.1119/1.16445
-
Loeffler FJ, Pedrotti FL, Bandettini P. Faraday rotation in the undergraduate advanced laboratory. Am. J. Phys. 1990, 58:542-545. AJPIAS, 0002-9505, 10.1119/1.13164, AJPIAS, 0002-9505, 10.1119/1.16445
-
(1990)
Am. J. Phys.
, vol.58
, pp. 542-545
-
-
Loeffler, F.J.1
Pedrotti, F.L.2
Bandettini, P.3
-
4
-
-
0003978119
-
-
(Addison-WesleyReadingMA)
-
Rossi B. Optics 1957, 427-430. (Addison-Wesley, Reading, MA)
-
(1957)
Optics
, pp. 427-430
-
-
Rossi, B.1
-
5
-
-
22944440687
-
Calculation of Verdet constants with time-dependent density functional theory: Implementation and results for small molecules
-
074105, JCPSA60021-960610.1063/1.459506JCPSA60021-960610.1063/1.1850919Seefor example
-
Bishop DMCybulski SMKrykunov MBanerjee AZiegler TAutschbach J. Calculation of Verdet constants with time-dependent density functional theory: Implementation and results for small molecules. J. Chem. Phys. 2005112:074105-1-7. JCPSA60021-960610.1063/1.459506JCPSA60021-960610.1063/1.1850919Seefor example and,.
-
(2005)
J. Chem. Phys.
, vol.112
, pp. 1-7
-
-
Bishop, D.M.1
Cybulski, S.M.2
Krykunov, M.3
Banerjee, A.4
Ziegler, T.5
Autschbach, J.6
-
7
-
-
0012640470
-
Theory of Faraday rotation produced by atoms near a Jg=12→Jg=12 transition
-
OPCOB80030-401810.1016/0030-4018(89)90305-2JPAPEH0953-407510.1088/0953-4 075/28/17/016and,. This paper also includes collisional and saturation effects.
-
Schuller FMacPherson MJ DStacey DNSchuller FStacey DNWarrington RBZetie KP. Theory of Faraday rotation produced by atoms near a Jg=12→Jg=12 transition. J. Phys. B 199528:3783-3790. OPCOB80030-401810.1016/0030-4018(89)90305-2JPAPEH0953-407510.1088/0953-4 075/28/17/016and,. This paper also includes collisional and saturation effects.
-
(1995)
J. Phys. B
, vol.28
, pp. 3783-3790
-
-
Schuller, F.1
MacPherson, M.J.D.2
Stacey, D.N.3
Schuller, F.4
Stacey, D.N.5
Warrington, R.B.6
Zetie, K.P.7
-
8
-
-
77950849476
-
-
022).
-
022).
-
-
-
-
9
-
-
19644367411
-
Two-level approximation in atomic systems
-
AJPIAS0002-950510.1119/1.1987910
-
Berman PR. Two-level approximation in atomic systems. Am. J. Phys. 197442:992-997. AJPIAS0002-950510.1119/1.1987910 .
-
(1974)
Am. J. Phys.
, vol.42
, pp. 992-997
-
-
Berman, P.R.1
-
10
-
-
77950823120
-
-
Because the equations of motion for the displacement operator of a harmonic oscillator contain a source term that is linear in the external electric fielda perturbative calculation of the Heisenberg operator r(t) yields a result that is correct to all orders in the electric field amplitude.
-
Because the equations of motion for the displacement operator of a harmonic oscillator contain a source term that is linear in the external electric fielda perturbative calculation of the Heisenberg operator r(t) yields a result that is correct to all orders in the electric field amplitude.
-
-
-
-
11
-
-
0021387978
-
Interaction Hamiltonian of quantum optics
-
JOBPDE0740-322410.1364/JOSAB.1.000116Seefor example
-
Ackerhalt JRMilonni PW. Interaction Hamiltonian of quantum optics. J. Opt. Soc. Am. B 19841:116-120. JOBPDE0740-322410.1364/JOSAB.1.000116Seefor example
-
(1984)
J. Opt. Soc. Am. B
, vol.1
, pp. 116-120
-
-
Ackerhalt, J.R.1
Milonni, P.W.2
-
12
-
-
77950827334
-
-
H2 [Eq. ]plus a term corresponding to the quadratic Zeeman shift.
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H2 [Eq. ]plus a term corresponding to the quadratic Zeeman shift.
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