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ISOTOPE SHIFT
EXPERIMENT
Nuclear Physics-1
SYEDA NIMRA SALAMAT
Isotope shift:
28-12-2020SYEDA NIMRA SALAMAT2
‘’ A displacement or splitting of spectral lines
indicating the presence of isotopes of an
element.”
Isotope shifts in atomic spectra are minute differences between the
electronic energy levels of different isotopes of the same element. If
atomic spectra also have hyperfine structure the shift refers to the
centre of gravity of the spectra.
Types of Isotope Shift:
MM.DD.20XXSYEDA NIMRA SALAMAT3
Mass Shift
(MS)
• In the lighter nuclei the MS is the
dominant shift that takes place, this
is due to the finite mass of the nuclei.
• The MS is due to the change in
kinetic energy of the nucleus, which
in turn depends on the nuclear mass.
Field Shift
(FS)
• In the heavier nuclei, the FS is
dominant, this is because of the none
zero nuclear volume. It is the field
shift, which provides information on
the radial parameters of the nucleus
and is therefore the part of interest in
nuclear physics.
• The FS is due to the change in the
spatial distribution of the nuclear
charge between isotopes.
Mass Shift (MS);
MM.DD.20XX
SYEDA NIMRA SALAMAT
4
1. Normal Mass Shift
(NMS)
• The NMS is due to the
difference in the reduced mass of
the electron-nucleus system and
is readily calculated.
2. Specific Mass Shift
(SMS)
• The SMS is due to momentum
correlations among electrons and
is not readily calculated.
Explanation:
MM.DD.20XX
SYEDA NIMRA SALAMAT
5
The technology of isotope shift covers many fields in chemistry, physics
, biology and even semiconductor technology. The main instrument used
in finding isotope shifts is the Spectroscope, this is an instrument that
breaks up a beam of light or other electromagnetic wave into the various
colours or wavelengths which are present, allows measurement of the
wavelengths of the various components. For visible light, the light is
normally broken up or dispersed with either a strong prism or a
diffraction grating.
ISOTOPE SHIFT Experiment:
MM.DD.20XX
SYEDA NIMRA SALAMAT
6
There are many experiments that have been done using isotope
shift technology. One of the main ones would be to see the
1. Isotope shift in the spectra of hydrogen and deuterium
2. Isotope effects in sonoluminescene
It is now known that most elements in nature consists of two or
more isotopes with the exception of beryllium, aluminium, phosphorus
and sodium. The latest research being done using isotope shift is as
various as the subject itself.
1. Isotope shift in the spectra of hydrogen and deuterium;
MM.DD.20XX
SYEDA NIMRA SALAMAT
7
The mass effect explains the isotope shift of Hydrogen/Deuterium quite well.
Because this shift is quite large, approximately 1 Å, it can be observed also in the
case of Doppler-broadened lines. An estimate of the isotope shift can be obtained
from: (RH und RD are the Rydberg constants for Hydrogen and Deuterium,
respectively)
𝑅 𝐷
𝑅 𝐻
=
1+
𝑚 𝑒
𝑚 𝐻
1+
𝑚 𝑒
𝑚 𝐷
≈ (1+
𝑚 𝑒
𝑚 𝐻
)(1−
𝑚 𝑒
𝑚 𝐷
)
or with 𝑚 𝐷 ≈ 2𝑚 𝐻 𝑎𝑛𝑑
𝑚 𝑒
𝑚 𝐻
≈
1
1836
:
𝑅 𝐷
𝑅 𝐻
≈ 1 +
𝑚 𝑒
2𝑚 𝐻
= 1 +
1
2.1836
MM.DD.20XX
SYEDA NIMRA SALAMAT
8
and
𝑣 𝐷 = 𝑅 𝐷(
1
𝑛2 −
1
𝑛2) = 𝑅 𝐻 1 +
𝑚 𝑒
2𝑚 𝐻
1
𝑛2 −
1
𝑛2 = 𝑣 𝐻(1 +
1
2.1836
)
or
𝜆 𝐷 = 𝜆 𝐻 1 −
1
2.1836
and
∆𝜆 = 𝜆 𝐻 − 𝜆 𝐷 = 𝜆 𝐻 (
1
2.1836
)
It is clear that the Deuterium lines are shifted to shorter wavelengths. The magnitude
of the shift is proportional to the wavelength.
MM.DD.20XXSYEDA NIMRA SALAMAT9
2. Isotope effects in sonoluminescene;
MM.DD.20XX
SYEDA NIMRA SALAMAT
10
The only pure liquids in which sonoluminescence (is a
phenomenon that occurs when a small gas bubble is periodically driven
in a liquid solution at ultrasonic frequencies, resulting in bubble
collapse, and light emission) from a single stable bubble has been
observed are water and heavy water. With regard to the content of the
trapped bubble there are a number of gases which yield light. Helium is
particularly interesting because its spectrum is strongly peaked in the far
ultraviolet. In order to learn about the mechanism responsible for
sonoluminescence, the search is on for differences between the spectra
of He[sup 4] and He[sup 3] bubbles in water and heavy water.
MM.DD.20XXSYEDA NIMRA SALAMAT11
Single-Bubble Multi-Bubble
MM.DD.20XX
SYEDA NIMRA SALAMAT
12
CONCLUSION:
MM.DD.20XXSyeda Nimra Salamat13
The understanding of atomic isotope shifts relies partly on the knowledge
of nuclear structure and provide information of the structure of nuclei. The
analyses of isotope shifts are similar to those of hyperfine structures in that
they consist of two steps.
 First, through the parametric study of the level energies, the angular
wavefunctions of the levels in intermediate coupling are determined.
 Second, through least-squares fitting procedure, the values of the isotope
shift parameters are adjusted so that experimental shift values can be
reproduced in the most accurate way.
The isotope shift is the sum of two terms: the mass effect and the field effect.
If only one isotope pair is available, the experiment only yields this sum but
not the respective contributions of the two effects.
HOPE FOR THE BEST
MM.DD.20XX
SYEDA NIMRA SALAMAT
14
THANK YOU 

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Isotope shift experiment

  • 2. Isotope shift: 28-12-2020SYEDA NIMRA SALAMAT2 ‘’ A displacement or splitting of spectral lines indicating the presence of isotopes of an element.” Isotope shifts in atomic spectra are minute differences between the electronic energy levels of different isotopes of the same element. If atomic spectra also have hyperfine structure the shift refers to the centre of gravity of the spectra.
  • 3. Types of Isotope Shift: MM.DD.20XXSYEDA NIMRA SALAMAT3 Mass Shift (MS) • In the lighter nuclei the MS is the dominant shift that takes place, this is due to the finite mass of the nuclei. • The MS is due to the change in kinetic energy of the nucleus, which in turn depends on the nuclear mass. Field Shift (FS) • In the heavier nuclei, the FS is dominant, this is because of the none zero nuclear volume. It is the field shift, which provides information on the radial parameters of the nucleus and is therefore the part of interest in nuclear physics. • The FS is due to the change in the spatial distribution of the nuclear charge between isotopes.
  • 4. Mass Shift (MS); MM.DD.20XX SYEDA NIMRA SALAMAT 4 1. Normal Mass Shift (NMS) • The NMS is due to the difference in the reduced mass of the electron-nucleus system and is readily calculated. 2. Specific Mass Shift (SMS) • The SMS is due to momentum correlations among electrons and is not readily calculated.
  • 5. Explanation: MM.DD.20XX SYEDA NIMRA SALAMAT 5 The technology of isotope shift covers many fields in chemistry, physics , biology and even semiconductor technology. The main instrument used in finding isotope shifts is the Spectroscope, this is an instrument that breaks up a beam of light or other electromagnetic wave into the various colours or wavelengths which are present, allows measurement of the wavelengths of the various components. For visible light, the light is normally broken up or dispersed with either a strong prism or a diffraction grating.
  • 6. ISOTOPE SHIFT Experiment: MM.DD.20XX SYEDA NIMRA SALAMAT 6 There are many experiments that have been done using isotope shift technology. One of the main ones would be to see the 1. Isotope shift in the spectra of hydrogen and deuterium 2. Isotope effects in sonoluminescene It is now known that most elements in nature consists of two or more isotopes with the exception of beryllium, aluminium, phosphorus and sodium. The latest research being done using isotope shift is as various as the subject itself.
  • 7. 1. Isotope shift in the spectra of hydrogen and deuterium; MM.DD.20XX SYEDA NIMRA SALAMAT 7 The mass effect explains the isotope shift of Hydrogen/Deuterium quite well. Because this shift is quite large, approximately 1 Å, it can be observed also in the case of Doppler-broadened lines. An estimate of the isotope shift can be obtained from: (RH und RD are the Rydberg constants for Hydrogen and Deuterium, respectively) 𝑅 𝐷 𝑅 𝐻 = 1+ 𝑚 𝑒 𝑚 𝐻 1+ 𝑚 𝑒 𝑚 𝐷 ≈ (1+ 𝑚 𝑒 𝑚 𝐻 )(1− 𝑚 𝑒 𝑚 𝐷 ) or with 𝑚 𝐷 ≈ 2𝑚 𝐻 𝑎𝑛𝑑 𝑚 𝑒 𝑚 𝐻 ≈ 1 1836 : 𝑅 𝐷 𝑅 𝐻 ≈ 1 + 𝑚 𝑒 2𝑚 𝐻 = 1 + 1 2.1836
  • 8. MM.DD.20XX SYEDA NIMRA SALAMAT 8 and 𝑣 𝐷 = 𝑅 𝐷( 1 𝑛2 − 1 𝑛2) = 𝑅 𝐻 1 + 𝑚 𝑒 2𝑚 𝐻 1 𝑛2 − 1 𝑛2 = 𝑣 𝐻(1 + 1 2.1836 ) or 𝜆 𝐷 = 𝜆 𝐻 1 − 1 2.1836 and ∆𝜆 = 𝜆 𝐻 − 𝜆 𝐷 = 𝜆 𝐻 ( 1 2.1836 ) It is clear that the Deuterium lines are shifted to shorter wavelengths. The magnitude of the shift is proportional to the wavelength.
  • 10. 2. Isotope effects in sonoluminescene; MM.DD.20XX SYEDA NIMRA SALAMAT 10 The only pure liquids in which sonoluminescence (is a phenomenon that occurs when a small gas bubble is periodically driven in a liquid solution at ultrasonic frequencies, resulting in bubble collapse, and light emission) from a single stable bubble has been observed are water and heavy water. With regard to the content of the trapped bubble there are a number of gases which yield light. Helium is particularly interesting because its spectrum is strongly peaked in the far ultraviolet. In order to learn about the mechanism responsible for sonoluminescence, the search is on for differences between the spectra of He[sup 4] and He[sup 3] bubbles in water and heavy water.
  • 13. CONCLUSION: MM.DD.20XXSyeda Nimra Salamat13 The understanding of atomic isotope shifts relies partly on the knowledge of nuclear structure and provide information of the structure of nuclei. The analyses of isotope shifts are similar to those of hyperfine structures in that they consist of two steps.  First, through the parametric study of the level energies, the angular wavefunctions of the levels in intermediate coupling are determined.  Second, through least-squares fitting procedure, the values of the isotope shift parameters are adjusted so that experimental shift values can be reproduced in the most accurate way. The isotope shift is the sum of two terms: the mass effect and the field effect. If only one isotope pair is available, the experiment only yields this sum but not the respective contributions of the two effects.
  • 14. HOPE FOR THE BEST MM.DD.20XX SYEDA NIMRA SALAMAT 14 THANK YOU 