ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM,...
Transcript of ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM,...
![Page 1: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/1.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
Website: www.physicsbyfiziks.com | Email: [email protected]
340
ATOMIC AND MOLECULAR PHYSICS
NET/JRF (JUNE-2011)
Q1. Consider the energy level diagram (as shown in the figure below) of a typical three level
ruby laser system with 1.6 1019 Chromium ions per cubic centimeter. All the atoms
excited by the 0.4 μm radiation decay rapidly to level 2E , which has a lifetime = 3 ms.
A. Assuming that there is no radiation of wavelength 0.7 μm present in the pumping
cycle and that the pumping rate is R atoms per cm3, the population density in the level N2
builds up as:
(a) N2 (t) = R(et/ –1) (b) N2 (t) = R(1 – e-t/)
(c)
/2
2 1 teRt
tN (d) N2 (t) = R t
Ans. : (b)
Solution: /2 1 tN t R e
B. The minimum pump power required (per cubic centimeter) to bring the system to
transparency, i.e. zero gain, is
(a) 1.52 kW (b) 2.64 kW (c) 0.76 kW (d) 1.32 kW
Ans. : (c)
Solution: The Minimum Power required to achieve zero gain is
hcNhvN
P22
336
83419
754103107.0
103106.6
2
106.1
cmW
kWP 76.0 per cubic centimeter
m4.0
m7.01E
2E
3E
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fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
Website: www.physicsbyfiziks.com | Email: [email protected]
341
NET/JRF (DEC-2011)
Q2. Given that the ground state energy of the hydrogen atom is –13.6 eV, the ground state
energy of positronium (which is a bound state of an electron and a positron) is
(a) + 6.8 eV (b) – 6.8 eV (c) – 13.6 eV (d) – 27.2 eV
Ans. : (b)
Solution: The energy expression for Positronium atom is eVn
En 22
6.13
For n = 1, eVeVE 8.62
6.131
, eVE 8.61
Q3. A laser operating at 500 nm is used to excite a molecule. If the Stokes line is observed at
770 cm-1, the approximate positions of the Stokes and the anti-Stokes lines are
(a) 481.5 nm and 520 nm (b) 481.5 nm and 500 nm
(c) 500 nm and 520 nm (d) 500 nm and 600 nm
Ans. :
Solution: Given 50 500 5 10nm cm , 1770 cmvstoke 1
0 20,000cm
Raman shift 10 19230 cmvvv stoke
Wave number of anti-stokes line is - 0anti stokev v v = 39,230 cm-1
In wavelength term nmstokeanti 9.25410549.2 7 and nmstoke 12987
Q4. If the hyperfine interaction in an atom is given by pe SSaH where eS and pS denote
the electron and proton spins, respectively, the splitting between the 13S and 0
1S state is
(a) 2/2a (b) 2a (c) 2/2a (d) 22 a
Ans. : (b)
Solution: Total spin is pe SSS
pepe SSSSS
2222 222
2
1pepe SSSSS
pe SSaH
222
2 pe SSSa
where 2222
4
31 SSSS pe
22222
2
3
24
3
4
3
2 S
aS
aH
For 2221
3 211: SSSSS , For 2220
1 010: SSSSS
221 42
32
2 aa
H
for 1
3 S and 222 4
3
2
30
2 a
aH
for 0
1 S
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H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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342
The splitting between 13 S and 0
1 S is 2221 4
3
4
1 aaHHH
Q5. The ratio of intensities of the D1 and D2 lines of sodium at high temperature is
(a) 1:1 (b) 2:3 (c) 1:3 (d) 1:2
Ans. : (d)
Solution: The electronic transition for D2 and D1 line is
2 22 3/ 2 1/ 2:D P S , 2 2
1 1/ 2 1/ 2:D P S 1
2
2
4
12
12
12
32
12
12
1
2
1
2
J
J
DI
DI
Q6. An atom of mass M can be excited to a state of mass M by photon capture. The
frequency of a photon which can cause this transition is
(a) h
c
2
2 (b)
h
c2 (c)
Mh
c
2
22 (d) M
Mh
c2
2
2
Ans. : (d)
Solution: The conservation law of energy and momentum give
2/122422 cpcMhMc and pc
h
224424222242 22 hcMccMhMchcM 4422 22 cMchMc
McMhMc
2122 42
Mh
c
21
2
MMh
c2
2
2
.
NET/JRF (JUNE-2012)
Q7. The first absorption spectrum of 12C16O is at 3.842 cm-1 while that of 13C16O is at
3.673 cm-1. The ratio of their moments of inertia is
(a) 1.851 (b) 1.286 (c) 1.046 (d) 1.038
Ans. : (c)
Solution: For 12 16 1 11 1: 2 3.842 1.921C O B cm B cm
For 12
12
1613 8365.1673.32: cmBcmBOC
Where, IC
hB
28 046.1
8365.1
921.1
2
1
1
2 B
B
I
I
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H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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343
Q8. The spin-orbit interaction in an atom is given by H aL S , where L and S denote the
orbital and spin angular momenta, respectively, of the electron. The splitting between the
levels 2P3/2 and 2P1/2 is
(a) 2
2
3 a (b) 2
2
1 a (c) 23 a 2 (d) 2
2
5 a
Ans. : (a)
Solution: Given SLaH where SLJ
.
2 2 2 2J L S L S
222
2
1SLJSL
222
2SLJ
aH
For 23/ 2
1:
2P S which gives 2 2 23
14
S S S
L = 1 which gives 222 21 LLL
2
3J which gives 222
4
151 JJJ 2 2
1
15 32
2 4 4 2
a aH
For 21/ 2
1:
2P S which gives 222
4
31 SSS
L = 1 which gives 222 21 LLL
2
1J which gives 222
4
31 JJJ 22
2 4
32
4
3
2 a
aH
2 2 21 2
3
2 2
aH H H a a
Q9. The spectral line corresponding to an atomic transition from J = 1 to J = 0 states splits in
a magnetic field of 0.1 Tesla into three components separated by 1.6 10-3 Ǻ. If the zero
field spectral line corresponds to 1849 Ǻ, what is the g-factor corresponding to the J = 1
state? (You may use 4
0
102hc
cm)
(a) 2 (b) 3/2 (c) 1 (d) 1/2
Ans. : (c)
Solution: The Zeeman splitting is BgBgME BBJ for MJ = +1
Given, Zeeman splitting separations, 32
106.1 c
Å
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344
1
210
8
2106.1
101849
103
c 100.1404 10
00.11.01027.9
101404.010625.624
1034
B
Eg
B
NET/JRF (DEC-2012)
Q10. Consider the energy level diagram shown below, which corresponds to the molecular
nitrogen laser.
If the pump rate R is 1020 atoms cm-3 s-1 and the decay routes are as shown with
2021 ns and s 11 , the equilibrium populations of states 2 and 1 are, respectively,
(a) 1410 cm-3 and 12102 cm-3 (b) 12102 cm-3 and 1410 cm-3.
(c) 12102 cm-3 and 6102 cm-3 (d) zero and 1020 cm-3
Ans. : (b)
Solution: 21
22
N
Rdt
dN and
1
1
21
21
NN
dt
dN .
Under equilibrium condition 012 dt
dN
dt
dN
20 9 12 32 21 10 20 10 2 10N R cm
3149
3126
21
211 10
1020
10210
cmcmN
N
Q11. Consider a hydrogen atom undergoing a SP 12 transition. The lifetime tsp of the 2P
state for spontaneous emission is 1.6 ns and the energy difference between the levels is
10.2 eV. Assuming that the refractive index of the medium n0 = 1, the ratio of Einstein
coefficients for stimulated and spontaneous emission 2121 / AB is given by
(a) 0.683 × 1012 m3J-1s-1 (b) 0.146 × 10-12 Jsm-3 .
(c) 6.83 × 1012 m3J-1s-1 (d) 1.463 × 10-12 Jsm-3 .
R 21
1
1
2
0
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345
Ans. : (a)
Solution: 0 1n , eVE 2.10 and
2 3 2 2 31221
33 3 321 0 0
0.67 10B c c
A n E n
.
Q12. Consider a He-Ne laser cavity consisting of two mirrors of reflectivities R1 = 1 and
R2 = 0.98. The mirrors are separated by a distance d = 20 cm and the medium in between
has a refractive index n0 = 1 and absorption coefficient α = 0. The values of the
separation between the modes and the width p of each mode of the laser cavity are:
(a) kHzkHz p 24,75 (b) kHzkHz p 100,100
(c) MHzMHz p 4.2,750 (d) MHzMHz p 750,4.2
Ans. : (c)
Solution: Mode separation MHzdn
c750
2 0
where sec/103 8 mc , 220 10d m and 10 n .
Width of each modec
p t
2
1 where
d
c
eRRc
dnt
221
0
1ln
2.
Note: In this question, there is no need to calculate p . Since in the given options there
is only one option with MHz750 and i.e., option (c). You can calculate p without
calculator so use your common sense.
NET/JRF (JUNE-2013) Q13. A muon from cosmic rays is trapped by a proton to form a hydrogen-like atom.
Given that a muon is approximately 200 times heavier than an electron, the longest
wavelength of the spectral line (in the analogue of the Lyman series) of such an atom will
be
(a) o
A62.5 (b) o
A67.6 (c) o
A75.3 (d) o
A3.13
Ans. : (b)
Solution: In case of muonic atom, the reduce mass is ep
p mmm
mmm 180'
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346
21
21
'' 180
n
E
n
E
m
mE
en
where, eVE 6.131
For ground state of muonic atom n=1, 1'1 180EE
For first excited state of muonic atom n=2, 1'2 45EE
The longest wavelength of the photon corresponds to the transition between first and ground state
of muonic atom.
The energy difference between first excited and ground state is
JeVEEEE 191
'1
'2 1029381836135
In term of wavelength
hc
hvE o
1019
834
A67.61067.6102938
1031063.6
mE
hc
Q14. Consider the hydrogen-deuterium molecule HD. If the mean distance between the two
atoms is 0.08 nm and the mass of the hydrogen atom is 2/938 cMeV , then the energy
difference E between the two lowest rotational states is approximately
(a) eV110 (b) eV210 (c) eV2102 (d) eV310
Ans. : (b)
Solution: Rotational energy expression 2
21 1
8
hE J J AJ J
I
Difference between two lowest energy levels is 2E A
where 2 2
28 2
hA
I I
and 2rI
Here, HHH
HH
DH
DH MMM
MM
MM
MM
3
2
2
2
, 9383
2 MeV/c2
34 34 19 1611.01 10 -sec 1.01 10 10 -sec 6.3 10 -sec
1.6J eV eV
2926
2162
1008.0/109383
2sec103.6
mceV
eV
IE
3 29.2 10 10eV eV
Q15. The electronic energy levels in a hydrogen atom are given by 2/6.13 nEn eV. If a
selective excitation to the 100n level is to be made using a laser, the maximum
allowed frequency line-width of the laser is
(a) 6.5 MHz (b) 6.5 GHz (c) 6.5 Hz (d) 6.5 kHz
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347
Ans. : (b)
Solution: GHzn
heVn
EnE nn 5.6106.16.1326.132
/6.13 1933
2
.
Q16. Consider the laser resonator cavity shown in the figure.
If 1I is the intensity of the radiation at
mirror 1M and is the gain coefficient of the
medium between the mirrors, then the energy
density of photons in the plane P at a
distance x from 1M is
(a) 1 / xI c e (b) 1 / xI c e
(c) 1 / x xI c e e (d) 21 / xI c e
Ans. : (c)
NET/JRF (DEC-2013)
Q17. A perturbation 2aLVpert is added to the Hydrogen atom potential. The shift in the
energy level of the P2 state, when the effects of spin are neglected up to second order in
a , is
(a) 0 (b) 4222 aa (c) 22 a (d) 422
2
3 aa
Ans. : (c)
Solution: For P2 state, L=1
The shift in the energy due to perturbation 2aLVpert is
222 2)11(1)1( aaLaLE
Q18. A gas laser cavity has been designed to operate at m 5.0 with a cavity length of m1 .
With this set-up, the frequency is found to be larger than the desired frequency by 100 Hz.
The change in the effective length of the cavity required to retune the laser is
(a) m1210334.0 (b) m1210334.0 (c) m1210167.0 (d) m1210167.0
Ans. : (d)
Solution: 2 2
22 2 2
c c c cm m L L L L L
L L c L L L
6
128
0.5 10 1 1000.167 10
3 10
LL m
c
11 R
1M P2M
x
l
RR 2
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348
Q19. The spectroscopic symbol for the ground state of Al13 is 2/12 P . Under the action of a
strong magnetic field (when SL coupling can be neglected) the ground state energy
level will split into
(a) 3 levels (b) 4 levels (c) 5 levels (d) 6 levels
Ans. : (c)
Solution: In extremely strong magnetic field coupling between L-S breaks down. J is no longer a
valid quantum number.
The ground state energy level will have 2 1 2 1 6S L states, but 2 states are
degenerate. Therefore, total energy levels will be 5 .
NET/JRF (JUNE-2014)
Q20. A spectral line due to a transition from an electronic state p to an s state splits into three
Zeeman lines in the presence of a strong magnetic field. At intermediate field strengths
the number of spectral lines is
(a) 10 (b) 3 (c) 6 (d) 9
Ans. : (a)
Solution: For p state: 1, 1/ 2 : 1/ 2 & 3/ 2l s j .
This gives two spectral terms 2P3/2 & 2P1/2
For s state: l= 0, s = 1/2: j = 1/2 : This gives spectral terms 2S1/2
The terms 2P3/2 and 2S1/2 corresponding to J = 3/2 & J = 1/2 will break into 2J+1 Zeeman
levels, which is 4 and 2 respectively.
For 2P3/2 Mj = - 3/2 -1/2 +1/2 +3/2
For 2S1/2 Mj = -1/2 +1/2
The selection rule is ∆MJ = 0, ± 1 (MJ = 0 → MJ = 0 If ∆J = 0)
∆MJ = 0 gives π component, ∆MJ = ±1 gives σ component
Number of π component = 2, Numbers of + components = 2
Number of - components = 2
The terms 2P1/2 and 2S1/2 corresponding to J = 1/2 & J = 1/2 will break into 2J+1 Zeeman
levels, which is 2 & 2 respectively.
For 2P1/2 Mj = -1/2 +1/2, For 2S1/2 Mj = -1/2 +1/2
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349
The selection rule is ∆MJ = 0, ± 1 (MJ = 0 → MJ = 0 If ∆J = 0)
∆MJ = 0 gives π component, ∆MJ = ±1 gives σ component
Number of π component = 2, Numbers of + components = 1
Number of - components = 1
Thus, total number of Zeeman component = 10
Q21. A double slit interference experiment uses a laser emitting light of two adjacent
frequencies 1v and 212 vvv . The minimum path difference between the interfering
beams for which the interference pattern disappears is
(a) 12 vv
c
(b)
12 vv
c
(c) 122 vv
c
(d) 122 vv
c
Ans. : (c)
Solution: The condition of maximum intensity for interfering laser beam is: nd sin
The condition of dark intensity for interfering laser beam is:
2
1sin nd
For interference pattern to vanish, the minimum path difference should be /2
The spectral bandwidth of laser is defined as, 2
c
v 2c
v
For two closely spaced line of wavelength 1 and 2
2
1 2
1 2 2 1
2 1 2 1
11 1
c c cc cv
Since, for interference pattern to vanish for two closely spaced line of wavelength 1 and
2, the minimum path difference should be = 12222
c
v
c
Q22. How much does the total angular momentum quantum number J change in the transition
of 63dCr atom as it ionize to 42 3dCr ?
(a) Increases by 2 (b) Decreases by 2 (c) Decreases by 4 (d) Does not change
Ans. : (c)
Solution: In 63Cr d state
2 1 0 1 2LM
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350
In this configuration, 1
4 22
S and 2L
This is the case of more than half filled subshell, thus state with highest J value will
have the lowest energy.
The highest J - value is J L S y
Thus, the ground state spectral term for this configuration is 54D .
Now in 2 43Cr d
2 1 0 1 2LM
In this configuration, 1
4 22
S and 2L
Since this is the case of less than half filled subshell, thus, state with lowest J value will
have the lowest energy.
The lowest J - value is 5 2 2 0J L .
Thus the ground state spectral term for this configuration is the J - value decreases from
4J to 0J .
Thus correct answer is option (c).
NET/JRF (DEC-2014)
Q23. An atomic transition SP 11 in a magnetic field 1 Tesla shows Zeeman splitting. Given
that the Bohr magneton TJB /1027.9 24 , and the wavelength corresponding to the
transition is 250 nm, the separation in the Zeeman spectral lines is approximately
(a) 0.01 nm (b) 0.1 nm (c) 1.0 nm (d) 10 nm
Ans. : (a)
Solution: This is the case of Normal Zeeman effect. The Zeeman separation in terms of
frequency, B B
h
, where B is Bohr magneton
In terms of wavelength, 2 2
BB
c c h
29 24
8 34
250 10 9.27 10 / 1
3 10 / 6.625 10
m J T T
m s Js
123 10 0.003m nm
None of the answer is matching correctly. But best suitable answer is option (a)
![Page 12: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/12.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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351
Q24. If the leading anharmonic correction to the energy of thn vibrational level of a diatomic
molecule is 2
2
1
nxe with 001.0ex , the total number of energy levels possible
is approximately
(a) 500 (b) 1000 (c) 250 (d) 750
Ans. : (a)
Solution: The energy of anharmonic oscillator is 2
1 1
2 2v eE v x v
where max0, 1, 2, .....v v is vibrational quantum number
Now, max
0v
v v
dE
dv
max
12 0
2ex v
max
11 2
2ex v max
1 1 1 1500
2 2 2 2 0.001e e
vx x
Q25. The effective spin-spin interaction between the electron spin eS
and the proton spin pS
in the ground state of the Hydrogen atom is given by pe SSaH
. As a result of this
interaction, the energy levels split by an amount
(a) 2
2
1 a (b) 22 a (c) 2a (d) 2
2
3 a
Ans. : (c)
Solution: The Hamiltonian is given as e pH aS S
where eS and pS are electron and proton spin.
The coupling between eS and pS gives net resultant spin angular momentum
e pS S S
, 2 2 2 2 2 212
2e p e p e p e pS S S S S S S S S S
2 2 2
2 e p
aH S S S
where 2 21S S S , 2 21e e eS S S , 2 21p p pS S S
Since 1
2eS and 1
2pS 0, 1S 23
4a
214
a2
1/21 s
0F
1F
S
eS
pS
maxv v
E
![Page 13: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/13.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
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352
For 0S (singlet state), 2 21
3 3 30
2 4 4 4
aH a
For 1S (Triplet state), 2 2 22
3 3 12
2 4 4 4
aH a
2 22 1
1 3
4 4H H H a a 2H a
NET/JRF (JUNE-2015)
Q26. Of the following term symbols of the 2np atomic configurations, 1 3 3 30 0 1 2, , ,S P P P and
12D which is the ground state?
(a) 30P (b) 1
0S (c) 32P (d) 3
1P
Ans. (a)
Solution: According to Hund’s rules
(i) State with highest multiplicity has lowest energy
(ii) State with same multiplicity, the state with highest L will have lowest energy
(iii) State with same multiplicity and L value. The state with lowest J has lowest energy
(only if subshell is less than half filled) from the given states 1 3 3 3 10 0 1 2 2, , ,S P P P D
The 30P will have the lowest energy
Q27. A diatomic molecule has vibrational states with energies 1
2vE v
and rotational
states with energies 1jE Bj j , where v and j are non-negative integers . consider
the transitions in which both the initial and final states are restricted to 1v and 2j
and subject to the selection rules 1v and 1j . Then the largest allowed energy
of transition is
(a) 3B (b) B (c) 4B (d) 2 B
Ans. (c)
Solution: 11
2E v BJ J
For vibrational transition with 1v and rotational transition with J we get
initial final 2 1E E E B J
![Page 14: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/14.jpg)
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353
where J is lowest quantum number
According to question in rotational states, two transition is possible, one for
0 1J J and second for 1 2J J
But, second transition will have photon of higher energy
For 1 2J J
2 1 1 4E B B
NET/JRF (DEC-2015)
Q28. The LS configurations of the ground state of 12 13 17, ,Mg Al Cl and 18 Ar are respectively,
(a) 3 2 21 1/ 2 1/ 2, ,S P P and 1
0S (b) 3 2 21 3 / 2 3 / 2, ,S P P and 3
1S
(c) 1 2 20 1/ 2 3 / 2, ,S P P and 1
0S (d) 1 2 20 3 / 2 1/ 2, ,S P P and 3
1S
Ans. : (c)
Solution: 2 2 6 212 :1 2 2 3Mg s s p s
Ground state: 10S
13 2 2 6 2 1:1 2 2 3 3Al s s p s p
the terms are 1/ 22 p and 3/ 22 p . Since its less than half filled. Thus
Ground state: 1/ 22 p
17 2 2 6 2 5:1 2 2 3 3Cl s s p s p
The terms are 1/ 22 p and 3/ 22 p . Since it shell is more than half filled.
Thus Ground state: 3/ 22 p
18 2 2 6 2 6:1 2 2 3 3Ar s s p s p
Ground state: 10S
Q29. For a two level system, the population of atoms in the upper and lower levels are 183 10
and 180.7 10 , respectively. If the coefficient of stimulated emission is
5 3 33.0 10 / -m W s and the energy density is 39.0 / -J m Hz , the rate of stimulated
emission will be
(a) 16 16.3 10 s (b) 16 14.1 10 s (c) 16 12.7 10 s (d) 16 11.8 10 s
Ans. : None of the answer is matching.
![Page 15: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/15.jpg)
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354
Solution: The rate of stimulated emission is
22 21
dNN B u w
dt
where 3 3
18 5 52 21 3 2
3 10 , 3 10 3 10m m
N BW s J s
and 33
9.0 / 9.0J s
u w J m Hzm
318 5 24 12
2 33 10 3 10 9 8.1 10
dN m J ss
dt J s m
Q30. The first ionization potential of K is 4.34 eV , the electron affinity of Cl is 3.82 eV
and the equilibrium separation of KCl is 0.3 nm . Then energy required to dissociate a
KCl molecule into a K and a Cl atom is
(a) 8.62 eV (b) 8.16 eV (c) 4.28 eV (d) 4.14 eV
Ans. : (c)
Solution: Energy required to dissociate KCl is KCl K Cl
21929 191 2
2 90 12
1.6 1019 10 7.7 10 4.79
4 0.3 10
cq q NmV J eV
r c m
The band dissociation energy is the energy required to dissociate a molecule into its
component atom KCl K Cl
To find the energy required to dissociate KCl into K and Cl , we must add an electron
to the K ion, which releases the atomic potassium ionization energy. Remove one
electron from Cl ion which requires the atomic chlorine electron affinity energy
Given ionization energy of 4.34ieK E eV
Electron affinity of 3.82aiCl E eV
Thus the energy gained in the transformation from ion to atom is
4.34 3.82 0.52ie aiE E eV
Thus dissociation energy 4.79 0.52 4.27 eV
![Page 16: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/16.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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355
NET/JRF (JUNE-2016)
Q31. The ground state electronic configuration of 22Ti is 2 23 4Ar d s . Which state, in the
standard spectroscopic notations, is not possible in this configuration?
(a) 13F (b) 1
0S (c) 12D (d) 3
0P
Ans. : (a)
Solution: The spectroscopic term for 2d are obtained as
1 22, 2 4,3,2,1,0l l L
1 2
1 1, 0,1
2 2s s S
Now, 140, 4 4,S L J G
120, 2 2,S L J D
100, 0 0,S L J S
3 3 34 3 21, 3 4,3,2, , ,S L J F F F
3 3 32 1 01, 1 2,1,0, , ,S L J P P P
Thus 13F is not possible spectroscopic term of 2 23 4Ar d S
Q32. In a normal Zeeman Effect experiment using a magnetic field of strength 0.3 T , the
splitting between the components of a 660 nm spectral line is
(a) 12 pm (b) 10 pm (c) 8 pm (d) 6 pm
Ans. : (d)
Solution: 292 19
8 31
660 10 1.6 10 0.3
4 3 10 4 9.1 10
eB
c m
126.09 10 m 6 pm
Q33. The separation between the energy levels of a two-level atom is 2 eV . Suppose that
204 10 atoms are in the ground state and 207 10 atoms are pumped into the excited state
just before lasing starts. How much energy will be released in a single laser pulse?
(a) 24.6 J (b) 22.4 J (c) 98 J (d) 48 J Ans. : (d)
Solution: 202 1 3 10N N
Energy of laser pulse, 2 1
2
N NE h
20193 10
2 1.6 102
J 48E J
![Page 17: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/17.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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356
NET/JRF (DEC-2016)
Q34. In the L S coupling scheme, the terms arising from two non-equivalent p -electrons are
(a) 3 1 3 1 3, , , ,S P P D D (b) 1 3 1 1, , ,S S P D
(c) 1 3 3 3, , ,S S P D (d) 1 3 1 3 1 3, , , , ,S S P P D D
Ans. : (d)
Solution: For pp configuration
1 2
1 1, 0,1
2 2s s S
1 21, 1 0,1,2l l L
Thus
1 100, 0 0 ; orS L J S S
1 110, 1 1 ; orS L J P P
1 120, 2 2 ; orS L J D D
3 311, 0 1 ; orS L J S S
3 30,1,21, 1 0,1, 2 ; orS L J P P
3 31,2,31, 2 1, 2,3 ; orS L J D D
Thus spectroscopic terms are 1 3 1 3 1 3, , , ,S S P P D D
Q35. The total spin of a hydrogen atom is due to the contribution of the spins of the electron
and the proton. In the high temperature limit, the ratio of the number of atoms in the spin-
1 state to the number in the spin- 0 state is
(a) 2 (b) 3 (c) 1
2 (d)
1
3
Ans. : (b)
Solution:
The degeneracy of quantum level is 2 1F .
Thus, 1
0
2 1 33
2 1 1
F
F
21/ 2S
0F
1F (when spins are parallel)
(when spins are anti-parallel)
![Page 18: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/18.jpg)
fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
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357
Q36. A two level system in a thermal (black body) environment can decay from the excited
state by both spontaneous and thermally stimulated emission. At room temperature
300 K , the frequency below which thermal emission dominates over spontaneous
emission is nearest to
(a) 1310 Hz (b) 810 Hz (c) 510 Hz (d) 1110 Hz Ans. : (d)
Solution: At thermal equilibrium, the ratio of the number of spontaneous to stimulated emission
is given by
21
21
1kTAe
B u
; where 34
1423
1.054 10 .2.55 10 sec
1.38 10 / 300
J S
kT J K K
Now, for 13 1310 6.3 10 / secv Hz rad ,
1.62
21
11 5 1 4
Ae
B u
For 11 1110 6.3 10 / secv Hz rad ,
31.6 1021
21
1 1.03 1 0.03A
eB u
This ratio is less than one, thus stimulated thermal emission dominates over spontaneous
emission below all frequency of 1110 Hz
NET/JRF (JUNE-2017)
Q37. An atomic spectral line is observed to split into nine components due to Zeeman shift. If
the upper state of the atom is 32D then the lower state will be
(a) 32F (b) 3
1F (c) 31P (d) 3
2P
Ans. : (c)
Solution: The possible zeeman component for different transitions are:
(i) 3 32 2 :D F Total zeeman components are 12
(ii) 3 32 1 :D P Total zeeman components are 9
(iii) 3 32 2 :D P Total zeeman components are 12
31F state is not allowed because for 3F , possible ‘ J ’ values are 2, 3 and 4.
Only 3 32 1D P transition gives 9 components. Therefore, ground state is 3
1P .
Thus, correct option is (c).
![Page 19: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/19.jpg)
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358
Q38. If the coefficient of stimulated emission for a particular transition is 19 3 1 32.1 10 m W s
and the emitted photon is at wavelength 0
3000A , then the lifetime of the excited state is
approximately
(a) 20ns (b) 40ns (c) 80 ns (d) 100ns
Ans. : (c)
Solution: 3
213
21
8A h
B c
. Life time
3 3
321 21 21
1
8 8
c
A h B hB
310
34 19 3 1 3
3000 10
8 6.6 10 . . 2.1 10J s m w s
208
13
2.7 107.7 10 sec
3.5 10
80 secn
Q39. If the binding energies of the electron in the K and L shells of silver atom are 25.4keV
and 3.34 keV , respectively, then the kinetic energy of the Auger electron will be
approximately
(a) 22 keV (b) 9.3keV (c) 10.5keV (d) 18.7 keV
Ans. : (d)
Solution: . .K E Auger electron is . K L LK E E E E
2K LE E
25.4 2 3.34 keV
18.7keV
eAuger electorn
Vacuum level
L
K
h
![Page 20: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/20.jpg)
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359
NET/JRF (DEC - 2017)
Q40. Consider a system of identical atoms in equilibrium with blackbody radiation in a cavity
at temperature T . The equilibrium probabilities for each atom being in the ground state
0 and an excited state 1 are 0P and 1P respectively. Let n be the average number of
photons in a mode in the cavity that causes transition between the two states. Let 0 1W
and 1 0W denote, respectively, the squares of the matrix elements corresponding to the
atomic transitions 0 1 and 1 0 . Which of the following equations hold in
equilibrium?
(a) 0 0 1 1 1 0P nW PW (b) 0 0 1 1 1 0P nW PnW
(c) 0 0 1 1 1 0 1 1 0P nW PW PnW (d) 0 0 1 1 1 0 1 1 0P nW PW PnW
Ans. : (d)
Solution: In equilibrium condition the number of upward transitions must be equal to the number
of downward transition.
Rate of upward transition 0 0 1P nW
Rate of downward transition = Rate of spontaneous transitions + Rate of stimulated
transition 1 1 0 1 1 0PW PnW
Thus, at thermal equilibrium
0 0 1 1 1 0 1 1 0P nW PW PnW
Correct option is (d)
Q41. The Zeeman shift of the energy of a state with quantum numbers , ,L S J and Jm is
. .
1J B
z s
m BH L J g S J
J J
where B is the applied magnetic field, sg is the g -factor for the spin and
11.4B MHz Gh
, where h is the Planck constant. The approximate frequency shift of
the 0, 1S L and 1Jm state, at a magnetic field of 1G , is
(a) 10 MHz (b) 1.4 MHz (c) 5MHz (d) 2.8MHz
Ans. : (b)
0 1W 1 0W
0
1
![Page 21: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/21.jpg)
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360
Solution: .4 2
BeB e Bv B
m m h h
11.4 1 1.4zMH G G MHz
Q42. The separations between the adjacent levels of a normal multiplet are found to be
122 cm and 133 cm . Assume that the multiplet is described well by the L S coupling
scheme and the Lande’s interval rule, namely 1E J E J AJ , where A is a
constant. The term notaions for this multiplet is
(a) 30,1,2P (b) 3
2,3,4F (c) 33,4,5G (d) 3
1,2,3D
Ans. : (d)
Solution: 11 1 1 22E E J E J A J cm
12 2 1 2 33E E J E J A J cm
1 221
2 33
A JJ
A J
Thus, the J values for all those three levels are1,2,3 . The, corresponding terms are
31,2,3D .
Q43. If the fine structure splitting between the 23/ 22 P and 2
3/ 22 P levels in the hydrogen atom
is 10.4 cm , the corresponding splitting in 2Li will approximately be
(a) 11.2 cm (b) 110.8 cm (c) 132.4 cm (d) 136.8 cm
Ans. : (c)
Solution: 4E z
4 4
4 4
381
1LiLi
H H
E z
E z
181 81 0.4HLiE E cm
132.4Li
E cm
Thus, correct option is (c).
2E
1E
2J
1J
J
![Page 22: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/22.jpg)
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361
NET/JRF (JUNE-2018)
Q44. Two Stern-Gerlach apparatus 1S and 2S are kept in a line ( x -axis). The directions of
their magnetic fields are along the positive z and y -axes, respectively. Each apparatus
only transmits particles with spins aligned in thee direction of its magnetic field. If an
initially unpolarized beam of spin 1
2 particles passes through this configuration, the ratio
of intensities 0 : fl l of the initial and final beams is
(a) 16 :1 (b) 2 :1 (c) 4 :1 (d) 1: 0
Ans. : (c)
Solution: 0
4f
II 0 4
1f
I
I
Q45. A photon of energy 115.62 keV ionizes a K -shell electron of a Be atom. One L -shell
electron jumps to the K -shell to fill this vacancy and emits a photon of energy
109.2 keV in the process. If the ionization potential for the L -shell is 6.4 keV , the
kinetic energy of the ionized electron is
(a) 6.42keV (b) 12.82keV (c) 20eV (d) 32eV
Ans. : (c)
Solution: Binding energy of K -shell electron
6.4 109.2 115.6pI KeV KeV KeV
Thus, K.E. of ionized electron is
=115.62 115.6 0.02 20KeV KeV KeV eV
Q46. The value of the Lande g -factor for a fine-structure level defined by the quantum number
1, 2L J and 1S , is
(a) 11
6 (b)
4
3 (c)
8
3 (d)
3
2
Ans. : (d)
0l k j fl
6.4 KeV
pI
L
109.2 KeV
K
e
115.6 KeV
![Page 23: ATOMIC AND MOLECULAR PHYSICS · 2021. 8. 7. · fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics H.No. 40-D, Ground Floor, Jia Sarai, Near](https://reader036.fdocuments.in/reader036/viewer/2022070300/6147f4b7a830d0442101c559/html5/thumbnails/23.jpg)
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362
Solution:
1 1 1
12 1
J J S S L Lg
J J
2 2 1 2 2 1 3
1 12 2 2 1 2 2
Q47. The electronic energy level diagram of a molecule is shown in the following figure,
Let ij denote the decay rate for a transition from the level i to j . The molecules are
optically pumped from level 1 to 2 . For the transition from level 3 to level 4 to be a
lassing transition, the decay rates have to satisfy
(a) 21 23 41 34 (b) 21 41 23 34
(c) 41 23 21 34 (d) 41 21 34 23
Ans. : (c)
Solution: The state 3 is metastable state, therefore 34 would be lowest to enhance population
inversion 41 23 . Thus correct sequence is 41 23 21 34
NET/JRF (DEC - 2018)
Q48. At low temperatures, in the Debye approximation, the contribution of the phonons to the
heat capacity of a two dimensional solid is proportional to
(a) 2T (b) 3T (c) 1/ 2T (d) 3/ 2T
Ans. : (a)
Solution: The dispersion relation of phonons is AK
The phonon specific heat in d -dimension is dVC T
For 2 dimensional solid 2d
2VC T
2
1
21
23
34
41
4
3Laser light
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fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
Website: www.physicsbyfiziks.com | Email: [email protected]
363
Q49. Barium Titanate 3BaTiO crystal has a cubic perovskite
structure, where the 2Ba ions are at the vertices of a unit
cube, the 2O ions are at the centres of the faces while the
2Ti is at the centre. The number of optical phonon modes of
the crystal is
(a) 12 (b)15
(c) 5 (d)18
Ans. : (a)
Solution: Effective number of atoms per unit cell is
1 18 6 1 1 1 3 1 5
8 2effn
Total degree of freedom 5 3 15
The number of Acoustical phonon modes 3
The number of optical phonon modes 15 3 12
Q50. The dispersion relation of optical phonons in a cubic crystal is given by 20k ak
where 0 and a are positive constants. The contribution to the density of states due to
these phonons with frequencies just below 0 is proportional to
(a) 1/ 2
0 (b) 3/ 2
0 (c) 2
0 (d) 0
Ans. : (a)
Solution: 3 3
24 42 2
L Lg k dk k dk k kdk
Given 1/ 220 0
1ak k
a and 2d akdk
3
1/ 2
03/ 2
4
2 2
Lg d
a
Thus, 1/ 2
0
4Ti 2Ba 2O
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fiziks Institute for NET/JRF, GATE, IIT‐JAM, M.Sc. Entrance, JEST, TIFR and GRE in Physics
H.No. 40-D, Ground Floor, Jia Sarai, Near IIT, Hauz Khas, New Delhi-110016 Phone: 011-26865455/+91-9871145498
Website: www.physicsbyfiziks.com | Email: [email protected]
364
Q51. A silicon crystal is doped with phosphorus atoms. (The binding energy of a H atom
is13.6 eV , the dielectric constant of silicon is 12 and the effective mass of electrons in
the crystal is 0.4 em ). The gap between the donor energy level and the bottom of the
conduction band is nearest to
(a) 0.01 eV (b) 0.08 eV (c) 0.02 eV (d) 0.04 eV
Ans. : (d)
Solution: *
2
13.6d
e
ME eV
M
2
13.60.4 0.04
12dE eV