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HYPERFINE SPLITTING Its role in Atomic transition
Roll no: 15251510-002
DEFINITION
Interaction between electron spin and nuclear spin is known as hyperfine interaction and
splitting occur due to this interaction is called hyperfine splitting.
When the electron spin interacts with nuclear spin then each electron spin state split into 2I+1
level this is known as hyperfine splitting.
RULES TO DETERMINE NUCLEAR SPIN:
 A nucleus with an even number of proton and even no of neutron has zero spin I= 0
for example 𝑐12,𝑂16, 𝐻𝑒4, 𝑆32, 𝐼 = 0
 A Nucleus with an odd number of proton and odd no of neutron has an integral spin.
for example 𝐻1, 𝑁14, 𝐼 = 1, 𝐵10, I = 3
 A nucleus with an odd mass has half integral spin
for example 𝐻1
, 𝐶13
, 𝑃31
, 𝐼 =
1
2
, 𝐶𝑈65
, 𝐼 =
3
2
CONT….
I= nuclear spin quantum no
The nuclear spin can have several orientations
for example;
I=1 , may have 𝑚𝑖=+1,0,-1
I=1/2 may have 𝑚𝑖 = +
1
2
, −
1
2
I=7/2 may have 𝑚𝑖 = +
7
2
, +
5
2
, +
3
2
, +
1
2
, −
7
2
, −
5
2
, −
3
2
, −
1
2
that is total of 2l+1
EXAMPLE: HYDROGEN
One unpaired electron (𝑚 𝑠 =
1
2
) of hydrogen interacts with its nuclear spin.
I value of H is ½, therefore 𝑚𝑖 = +
1
2
, −
1
2
.
Each 𝑚 𝑠state will interact with 𝑚𝑖value and split into 2I+1.
The energy of particular 𝑚 𝑠 𝑠tate will be affected by nuclear spin –electron spin
interaction energy.
This energy varies the product of 𝑚 𝑠 𝑎𝑛𝑑 𝑚𝑖, 𝑔𝑖𝑣𝑒𝑛 𝑏𝑦 𝐴𝑚 𝑠 𝑚𝑖. A is the hyperfine
splitting constant.
The energy of different levels are given by
𝐸 = 𝑔𝛽𝑚 𝑠 + 𝐴𝑚 𝑠 𝑚𝑖
CONT…
DEUTERIUM:
It has one unpaired electron(𝑚 𝑠 =
1
2
) interacts with nuclear spin.
I value of 𝐻2 𝑖𝑠 1, therefore 𝑚𝑖 = +1,0 𝑎𝑛𝑑 − 1.
2𝐼 + 1 = 2 × 1 + 1 = 3
APPLICATIONS:
Astrophysics:
In radio astronomy, heterodyne receivers are widely used in detection of the electromagnetic
signals from celestial objects. The separations among various components of a hyperfine
structure are usually small enough to fit into the receiver's IF band.
Nuclear technology:
The atomic vapor laser isotope separation (AVLIS) process uses the hyperfine splitting
between optical transitions in uranium-235 and uranium-238 to selectively photo-ionize only
the uranium-235 atoms and then separate the ionized particles from the non-ionized ones.
The hyperfine structure transition can be used to make a microwave notch filter with very
high stability, repeatability and Q factor, which can thus be used as a basis for very
precise atomic clocks.

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Hyperfine splitting

  • 1. HYPERFINE SPLITTING Its role in Atomic transition Roll no: 15251510-002
  • 2. DEFINITION Interaction between electron spin and nuclear spin is known as hyperfine interaction and splitting occur due to this interaction is called hyperfine splitting. When the electron spin interacts with nuclear spin then each electron spin state split into 2I+1 level this is known as hyperfine splitting.
  • 3. RULES TO DETERMINE NUCLEAR SPIN:  A nucleus with an even number of proton and even no of neutron has zero spin I= 0 for example 𝑐12,𝑂16, 𝐻𝑒4, 𝑆32, 𝐼 = 0  A Nucleus with an odd number of proton and odd no of neutron has an integral spin. for example 𝐻1, 𝑁14, 𝐼 = 1, 𝐵10, I = 3  A nucleus with an odd mass has half integral spin for example 𝐻1 , 𝐶13 , 𝑃31 , 𝐼 = 1 2 , 𝐶𝑈65 , 𝐼 = 3 2
  • 4. CONT…. I= nuclear spin quantum no The nuclear spin can have several orientations for example; I=1 , may have 𝑚𝑖=+1,0,-1 I=1/2 may have 𝑚𝑖 = + 1 2 , − 1 2 I=7/2 may have 𝑚𝑖 = + 7 2 , + 5 2 , + 3 2 , + 1 2 , − 7 2 , − 5 2 , − 3 2 , − 1 2 that is total of 2l+1
  • 5. EXAMPLE: HYDROGEN One unpaired electron (𝑚 𝑠 = 1 2 ) of hydrogen interacts with its nuclear spin. I value of H is ½, therefore 𝑚𝑖 = + 1 2 , − 1 2 . Each 𝑚 𝑠state will interact with 𝑚𝑖value and split into 2I+1. The energy of particular 𝑚 𝑠 𝑠tate will be affected by nuclear spin –electron spin interaction energy. This energy varies the product of 𝑚 𝑠 𝑎𝑛𝑑 𝑚𝑖, 𝑔𝑖𝑣𝑒𝑛 𝑏𝑦 𝐴𝑚 𝑠 𝑚𝑖. A is the hyperfine splitting constant. The energy of different levels are given by 𝐸 = 𝑔𝛽𝑚 𝑠 + 𝐴𝑚 𝑠 𝑚𝑖
  • 7. DEUTERIUM: It has one unpaired electron(𝑚 𝑠 = 1 2 ) interacts with nuclear spin. I value of 𝐻2 𝑖𝑠 1, therefore 𝑚𝑖 = +1,0 𝑎𝑛𝑑 − 1. 2𝐼 + 1 = 2 × 1 + 1 = 3
  • 8. APPLICATIONS: Astrophysics: In radio astronomy, heterodyne receivers are widely used in detection of the electromagnetic signals from celestial objects. The separations among various components of a hyperfine structure are usually small enough to fit into the receiver's IF band. Nuclear technology: The atomic vapor laser isotope separation (AVLIS) process uses the hyperfine splitting between optical transitions in uranium-235 and uranium-238 to selectively photo-ionize only the uranium-235 atoms and then separate the ionized particles from the non-ionized ones. The hyperfine structure transition can be used to make a microwave notch filter with very high stability, repeatability and Q factor, which can thus be used as a basis for very precise atomic clocks.