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ZERO-FIELD SPLITTING &
KRAMER’S DEGENERACY
     Compiled by: Yaseen Aziz

       Roll number: 23609

         M.Sc. Chemistry

          Semester 3rd
Zero–field splitting :-
 The splitting of spin levels even in the absence of
  magnetic field is called zero–field splitting.
 Occurs mainly in in transition metal complexes
  where there are more than one unpaired
  electrons.
 Removes the degeneracy of transitions and more
  transitions are observed than expected , in the presence
  of external magnetic field.
 Fine structure in ESR spectrum is obtained.
CAUSES & MECHANISM :

Dipolar interactions among electrons:
i.     In a d2 system, S=1 both electrons being parallel.
       Since each spin produces a small magnetic field in
       the vicinity of its partner. The dipolar
       interactions for mS=+1 and mS=-1 or same and
       mS=0 has different dipolar interaction than +1 or
       -1 states. Thus -1 and +1 mS states are raised than
       mS=0 state.
ii.    Spin orbit coupling
iii.    A strong internal electric field which results in the
       perturbations to the energy levels of mS=+1 and -1
       states but not of mS=0 state.
Kramer’s degeneracy /Rule :
 Crystal field lifts the spin degeneracy of two or more unpaired electrons
  in a complex due to electrostatic interactions (ZFS).
 When the species contains an odd number of unpaired electrons, the spin
  degeneracy of every level remains doubly degenerate. This is known as
  Kramer’s degeneracy.

           When the number of unpaired electrons is even, crystal field
           may remove the spin degeneracy entirely.

   This can be schematically represented as follows:
Odd number
                                 Kramer’s
                                degeneracy
                Magnetic      Applies and
              field if only    each level
   Spi n      1 electron is   must remain
                                 doubly
degener acy     present       degenerate
                              Even number
  can be       Crystal         Crystal field
              field if more   removes the
r emoved by                        spin
                  than 1
                unpaired      degeneracy
                              completely
               electron is
                                i.e. non-
                 present      degenerate
Some examples :
1. In a d2 system with two unpaired electrons, S = +½ + ½ = 1.
Therefore, ms= -1, 0, +1. In the absence of zero – field splitting, two transitions
are possible as shown below:




 The first transition is ms= 0 to +1 and the second transition is ms= -1 to 0.
 These transitions have equal energy (i.e. degenerate) and only one signal is
 observed. This system has even number of unpaired electrons. Hence,
 Kramer’s degeneracy is not operative. That is, each level will not be doubly
 degenerate.
If zero – field splitting is present, it removes the degeneracy in mS as
  shown below:



                                           zero-field splitting
 Subsequent magnetic field splits the levels further as shown below :




Here, two transitions are not degenerate. 2 peaks =>ZFS present, 1 peak =>ZFS
absent.
2. In a d5 system like Mn(2+), there is an odd number of unpaired electrons.
So, Kramer’s degeneracy is operative here. The term symbol for the free ion
ground state is S6. The zero – field splitting produces three doubly degenerate
spin states, namely, mS=+5/2,+3/2,+½ (Kramer ’s degeneracy).
Consequences of ZFS :
 Large ZFS => transitions fall out of the microwave region. e.g. In V(3+)
mS= 0 to mS= +1 transition is not observed. However, a weak transition
between mS= +1 and mS= -1 has been observed (forbidden).
 Number of peaks observed in the spectrum is more. The spectrum
   becomes much more complex when hyperfine splitting is also
   incorporated.
THANK
 YOU

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Zero field splitting

  • 1. ZERO-FIELD SPLITTING & KRAMER’S DEGENERACY  Compiled by: Yaseen Aziz  Roll number: 23609  M.Sc. Chemistry  Semester 3rd
  • 2. Zero–field splitting :-  The splitting of spin levels even in the absence of magnetic field is called zero–field splitting.  Occurs mainly in in transition metal complexes where there are more than one unpaired electrons.  Removes the degeneracy of transitions and more transitions are observed than expected , in the presence of external magnetic field.  Fine structure in ESR spectrum is obtained.
  • 3. CAUSES & MECHANISM : Dipolar interactions among electrons: i. In a d2 system, S=1 both electrons being parallel. Since each spin produces a small magnetic field in the vicinity of its partner. The dipolar interactions for mS=+1 and mS=-1 or same and mS=0 has different dipolar interaction than +1 or -1 states. Thus -1 and +1 mS states are raised than mS=0 state. ii. Spin orbit coupling iii. A strong internal electric field which results in the perturbations to the energy levels of mS=+1 and -1 states but not of mS=0 state.
  • 4. Kramer’s degeneracy /Rule :  Crystal field lifts the spin degeneracy of two or more unpaired electrons in a complex due to electrostatic interactions (ZFS).  When the species contains an odd number of unpaired electrons, the spin degeneracy of every level remains doubly degenerate. This is known as Kramer’s degeneracy. When the number of unpaired electrons is even, crystal field may remove the spin degeneracy entirely.  This can be schematically represented as follows:
  • 5. Odd number Kramer’s degeneracy Magnetic Applies and field if only each level Spi n 1 electron is must remain doubly degener acy present degenerate Even number can be Crystal Crystal field field if more removes the r emoved by spin than 1 unpaired degeneracy completely electron is i.e. non- present degenerate
  • 6. Some examples : 1. In a d2 system with two unpaired electrons, S = +½ + ½ = 1. Therefore, ms= -1, 0, +1. In the absence of zero – field splitting, two transitions are possible as shown below: The first transition is ms= 0 to +1 and the second transition is ms= -1 to 0. These transitions have equal energy (i.e. degenerate) and only one signal is observed. This system has even number of unpaired electrons. Hence, Kramer’s degeneracy is not operative. That is, each level will not be doubly degenerate.
  • 7. If zero – field splitting is present, it removes the degeneracy in mS as shown below: zero-field splitting Subsequent magnetic field splits the levels further as shown below : Here, two transitions are not degenerate. 2 peaks =>ZFS present, 1 peak =>ZFS absent.
  • 8. 2. In a d5 system like Mn(2+), there is an odd number of unpaired electrons. So, Kramer’s degeneracy is operative here. The term symbol for the free ion ground state is S6. The zero – field splitting produces three doubly degenerate spin states, namely, mS=+5/2,+3/2,+½ (Kramer ’s degeneracy).
  • 9. Consequences of ZFS :  Large ZFS => transitions fall out of the microwave region. e.g. In V(3+) mS= 0 to mS= +1 transition is not observed. However, a weak transition between mS= +1 and mS= -1 has been observed (forbidden).  Number of peaks observed in the spectrum is more. The spectrum becomes much more complex when hyperfine splitting is also incorporated.