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Zeeman spectrum of a Cm multiplet in TEXTOR for B 1.79T under longitudinal observation

Zeeman splitting for a nucleus with spin 7 3 2, v 0.

Zeeman splitting of an 5 2 paramagnet with D -0.5 cm , with the applied field along the molecular z axis

Zeeman splitting of an 5 2 paramagnet with D -0.5 cm and E 0.01 cm with the applied field along the molecular z axis. Inset

Zeeman splitting of an isotropic 5 2 paramagnet in an applied magnetic field

Zeeman splitting of energy levels of an electron placed in a magnetic field

Zeeman splitting of lines 1 . Copyright 1975 by the American Physical Society

Zeeman splitting of the 2p i line of P in diamond for B 111 . is 2-3x 1018 at cm 3 . Copyright Wiley-VCH Verlag GmbH Co. KGaA. Reproduced with permission

Zeeman splitting of the Af 1 and 2 rotational levels in the CN radical. In region 1 the rotational transition is electric dipole allowed and magnetically tunable. In region 3 the magneticaUy-tunable transitions are magnetic dipole electron spin transitions the electric dipole transitions are not magnetically tunable. Region 2 is intermediate between these limiting cases.

Zeeman splitting of the bound exciton line 14. Case

Zeeman splitting of the Ce 0 2 CEF states 1 and in a magnetic field parallel to a cubic axis.

Zeeman splitting of the J 1 rotational level of a A state, and the observed

Zeeman splitting of the J 2 rotational level of a A state, and the observed A Mj 1 transitions.

Zeeman splitting of the lowest AE octet of CH3 group. The levels of the E state with m are doubly degenerate.

Zeeman splitting of the lowest AE octet of the CH3 group. Levels of the E state with m 1 2 are twice degenerate.

Zeeman splitting of the lowest AE octet of the CHj group. Levels of the E state with m 1 2 are twice degenerate.

Zeeman splitting of the lowest triplet and singlet levels of positronium. The r.f. transition has been drawn, for clarity of illustration, at a higher field than that used by Deutsch and Brown

Zeeman splitting of the N 1 and 2 rotational levels in the CN radical. In region 1 the rotational transition is electric dipole allowed and magnetically tunable. In region 3 the magnetically-tunable transitions are magnetic dipole electron spin transitions the electric dipole transitions are not magnetically tunable. Region 2 is intermediate between these limiting cases.

Zeeman splitting of the nuclear ground and excited states of Both states have the same spin but the

Zeeman splitting, in an external magnetic field of 10 gauss, of the four-wave mixing resonance in the geometry of

Zeeman splittings and transitions between the T , T, and T0 triplet spin states for localized diradicals.

Zefirov topologies of reactions on three to six atoms

Zein enrichment with Trp, Thr, and Lys by a plastein reaction,

Zein powder.

Zeise s dimer catalyzed hydration annulation of Y-hydroxy-a, 3 -acetylenic esters



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