Research Areas

Gamma Detector Array

Gamma Detector Array

About Gamma Detector Array

The facility has twelve HPGe detectors placed coaxially in the 'anticompton shields' at 45o, 99o and 153o with respect to the beam direction in two horizontal rings at ± 25o to the horizontal plane. 14 BGO detectors, seven above and seven below the scattering chamber in the 'honey comb structure' arrangement, cover about 35% of total solid angle at the target. These are used as total energy and/or multiplicity filter.

GDA has a 18 cm diameter scattering chamber equipped with a target ladder, two view ports and a collimator. Oil free vacuum is maintained in the chamber by a turbo molecular pump.

The high density electronics facilitates to acquire data in singles and in multiparameter mode, through a CAMAC interface. Data taken, generally, include:

  • Energy information from two HPGe detectors which are at 99o and 153o (of opposite sides) in singles with or without multiplicity gate.
  • Hit pattern of twelve HPGe detectors in event mode.
  • Energy information from twelve HPGe detectors in event mode.
  • Hit pattern of the BGO detectors.
  • Time information from twelve HPGe detectors in event mode.


Recoil distance device (RDD)

The device, which has been in operation since 1994 for lifetime measurements (nanoseconds - picoseconds), was initially designed and fabricated by the Delhi University group. The RDD is routinely used in the GDA system along with the 14 element BGO multiplicity filter.

Recoil distance device

The main features of this device are as follows:

  • It consists of three PC controlled micro motors with a precision movement of one μm. The motors can be moved individually or together in a synchronised fashion.
  • The target holder assembly is mounted on three INVAR rods attached to the micro motors.
  • The stopper holder assembly is mounted on three INVAR rods fixed to the system.
  • A collimator is mounted 5 cm upstream the target and a Faraday cup is installed 15 cm downstream the target. Both are attached to the fixed INVAR rods.
  • The typical minimum distance achieved between the stretched target and the stopper is 10 μm.
  • The vacuum chamber of RDD is made of glass to allow visual inspection of the target-stopper assembly during the experiment.

Charged particle detector array (CPDA)

The array, which covers nearly 4π solid angles, has been fabricated for use in conjunction with GDA. It has large efficiency for detecting protons and α particles evaporated from neutron deficient nuclei in a nuclear reaction. The array consists of fourteen charged particle detectors (phoswich detector, optical guide, PMT base) along with required cables and electronics (buffer module and amplifier cum attenuator module). The scattering chamber includes a target ladder, collimator support, and current feedthrough.

Charged particle detector array

A full-fledged experiment with the full array was carried out to populate compound nucleus 79Rb by bombarding 110 MeV 28Si beam on 51V target. The proton and αa multiplicities, along with γ-γ coincidence spectra were recorded event by event. A large reduction in background was observed in particle gated spectra compared to singles (Eγ). The CPDA is suitable for identifying weak reaction channels and can be used for count rates upto 50,000 Hz. This project is funded by the Department of Science and Technology, Government of India.

Mini orange electron spectrometer (MOES)

This device is designed and fabricated by the Punjab University group. The spectrometer consists of five wedge shaped magnets with a thick lead absorber. For detecting the electrons, a Si(Li) detector is used. A facility test with the reaction 11B(124Sn, 5n)130Cs at 55 MeV beam energy was carried out in the GDA beamline with six Compton-suppressed germanium detectors. The conversion electrons from 130Cs were identified by gating with γs from the multiplicity filter. Now the facility is open for nuclear structure work at IUAC.

Mini orange electron spectrometer

Perturbed Angular Distribution (PAD) Setup

Ensemble of excited and aligned (perpendicular to the beam direction) nuclei is formed in nuclear reactions. The resulting anisotropic intensity distribution of γ-rays can be perturbed due to the extra-nuclear electromagnetic fields (through hyperfine interactions) depending on the lifetime of the excited state. The extracted perturbation factor, observed in the integral or differential mode concerning time, is proportional to the product of the nuclear parameter (magnetic and quadrupole moments) and the atomic environment (magnetic field and electric field gradient due to electronic spin and charge distribution). The PAD technique is a well-established technique in most accelerator laboratories because of the following reasons:

(i) The static electromagnetic moments (crucial for the unambiguous nuclear structure information) of the excited states can be measured only through this technique.

(ii) As compared to the Mossbauer and the NMR techniques this is a very sensitive technique. For the problems in condensed matter physics, one can have a very low concentration (to reduce the impurity – impurity interaction) of probe atoms of most of the elements with no limitation of the temperature.

The PAD facility at IUAC consists of an angular correlation table, target chamber, and a C-type electromagnet (to provide a maximum 1.8 T magnetic field between the 1” pole gap). Both types of detectors, scintillators, and semiconductors can be mounted in the plane perpendicular to the magnetic field. In the past, the main interest has been for the systematic investigations of the nuclear structure (configuration and the quadrupole deformation) and the decay mechanism of the K-isomers in the Hf-Ta region. Now the PAD setup is redesigned and the experiments are planned for the nuclear moment measurements using the transient magnetic fields and the ionic state of the transitional impurities in dilute magnetic semiconductors.


Annealing station

An oil free vacuum station based on turbo molecular pump and diaphragm pump is set up in the GDA laboratory for annealing and evacuating the cryostats of HPGe detectors. This system is protected against power failures with solenoid activated valve. This annealing system has become the work station for HPGe detector maintenance activities.

Annealing station

LN2 autofilling system

An automatic liquid nitrogen filling system has been designed and made in-house, with a dedicated controller which controls a set of electro-pneumatic valves/sensors to fill the 12 HPGe detectors in proper sequence and in failsafe mode. The temperature readout from the sensors (platinum resistor - PT100 whose resistance varies linearly with temperature) is communicated to the PC through the ADC in the controller. The controller also has the relays to operate the 24 V dc solenoids of electro-pneumatic valves.

LN2 autofilling system

The filling system consists of dedicated manifolds for liquid nitrogen and compressed air on both sides of the beamline each catering to 6 detectors. The detectors are periodically and automatically filled once a day. Fill log is maintained in a logfile for monitoring purposes. Filling is done from a 200 l capacity LN2 dewar (at a pressure of 22 psig) which itself gets filled from a 5000 l dewar kept outside the Beam Hall, once in 2 days. The process is controlled by a GUI code working in linux environment. The configuration of the number of detectors, sensors, valves (enabled/disabled) are kept in the file 'lnfill.conf'.

LN2 dewar


For the study of nuclear spectroscopy, the emphasis has mainly been on the study of the high spin structure of vibrational nuclei and nuclei near shell closure. The systematics of high spin levels in nuclei in the mass region ~ 75, ~ 90, ~ 120, ~ 130, and ~ 160 have been carried out in the last few years to investigate the interplay of a single particle, vibrational and rotational degrees of freedom, and the co-existence of these structures.

A systematic study of nuclei near N=50 shell closure was carried out to understand the evolution of high spin structure in these nuclei. In contrast to nuclei near Z=50 shell closure, measurements in 92,93,94,95Tc, 95,96,97,98Ru and 95Rh indicate that these nuclei do not develop any rotational behaviour at high spin. The low lying levels of these nuclei are well described in terms of large basis shell model calculations using the f-p-g valency nucleons. These calculations have been extended by incorporating proton and neutron core excitation in truncated model space. Calculations indicate that the levels up to J ~ 22 ħ and E* ~ 10 MeV can be attributed to the breaking of the N=50 core. Similar effects of core breaking for N=82 shell have been observed for the nucleus 149Dy. In contrast to N ~ 50 nuclei where the high spin structure is a single particle in nature, the Z=50 nucleus 111Sn shows a rotational band at high spin. The transitional nuclei 99Rh and 100Pd have been observed to have a well-defined rotational behaviour.

An extensive measurement of the transitional nuclei near A ~ 120 has been carried out using the GDA facility. High spin structures of the nuclei 120X, 116,118,119,121Te and 118,120I have been established. A systematic study of Te isotopes indicated the fully aligned P[(g9/2)2]6+N[(h11/2)2]10+ non-collective oblate configuration in 116,118Te.

The high spin structures of odd-odd Lu nuclei have been extensively studied. The energy levels of 164Lu through γ-spectroscopy have been established for the first time. Two strongly coupled bands were identified and tentatively assigned the configurations Ph11/2 [523]7/2- Ni13/2 [642]5/2+ and Ph11/2 [523]7/2- Nh9/2 [521]3/2-. The above assignments are consistent with the observed crossing frequencies, alignments and B(M1)/B(E2) ratios as compared to the neighbouring odd A nuclei. Measurements were also carried out for other odd-odd isotopes of Lu (162,168,170Lu) which show a gradual reduction of signature splitting with increasing neutron number.

Lifetime measurements in the γ-soft region (A ~ 70-80) have indicated a rapid change of nuclear shape with rotation and the shape polarisation effect of the occupied g9/2 proton and neutron orbitals. Identical bands have been observed in the nuclei 78Kr and 80Rb. The unraveling of the low spin structure, particularly the -ve parity sidebands, was facilitated by the use of the recoil mass separator.

A new high spin isomer (35/2-) with a lifetime of 8.6 ± 1.3 ns has been identified in 153Eu. Measurement of quadrupole moments of several nuclei has been carried out using the DSAM, RDM, and hyperfine interaction studies. The current emphasis is on complete nuclear spectroscopy using information from γ-γ, e-γ, and lifetime measurements.


Staff Telephone: +91 11 26893955, 26892601, 26892603 Telefax: +91 11 26893666


  • Jasmeet Kaur

    Department of Physics Panjab University, Chandigarh, India

  • Abhishek Yadav

    Department of Physics Aligarh Muslim University, Aligarh, India


  • Dinesh Negi

    Inter University Accelerator Centre New Delhi, India

  • Ritwika Chakraborty

    UGC-DAE CSR, Kolkata Centre Kolkata, India

  • Anukul Dhal

    Banaras Hindu University, Varanasi, India

  • Rishi Kumar Sinha

    Banaras Hindu University, Varanasi, India

  • Pushpendra P. Singh

    Aligarh Muslim University, Aligarh, India

  • Rahbar Ali

    Aligarh Muslim University, Aligarh, India

  • Vivek Chandel

    Punjab University, Chandigarh, India

  • Ajay Deo

    Mumbai University, Mumbai, India

  • Kuljeet Singh

    Punjab University, Chandigarh, India

  • V. Kumar

    Punjab University, Chandigarh, India

  • S.R. Kore

    Mumbai University, Mumbai, India

  • Somen Chanda

    Variable Energy Cyclotron Centre / Calcutta University, Kolkata, India

  • Hema Iyer

    Punjab University, Chandigarh, India

  • Vinod Kumar

    Indian Institute of Technology Mumbai Mumbai, India

  • S.K. Chamoli

    Punjab University, Chandigarh, India

  • R. Dogra

    Punjab University, Chandigarh, India

  • P. Thakur

    Punjab University, Chandigarh, India

  • B. Mukherjee

    Inter University Accelerator Centre New Delhi, India

  • P. Joshi

    Punjab University, Chandigarh, India

  • Indrani Ray

    Saha Institute of Nuclear Physics / Calcutta University, Kolkata, India

  • S. Bhattacharya

    Variable Energy Cyclotron Centre / Calcutta University, Kolkata, India

  • U.D. Pramanik

    Saha Institute of Nuclear Physics / Calcutta University, Kolkata, India

  • S.K. Katoch

    Delhi University, Delhi, India

  • S. Basu

    Saha Institute of Nuclear Physics / Calcutta University, Kolkata, India

  • G. Mukherjee

    Visvabharati University, Santiniketan, India

  • S.K. Tandel

    Mumbai University, Mumbai, India, India

  • Jagbir Singh

    Punjab University, Chandigarh, India

  • G. Gangopadhyay

    Calcutta University, Kolkata, India

  • V. Ravi Kumar

    Andhra University, Visakhapatnam, India

  • H. Kaur

    Punjab University, Chandigarh, India

  • M. Gupta

    Mumbai University, Mumbai, India

  • A. Sharma

    Punjab University, Chandigarh, India

  • J. Goswamy

    Punjab University, Chandigarh, India

  • S.S Ghugre

    Mumbai University, Mumbai, India


  • Enhanced 0+g.s. → 2+1 E2 Transition Strength in 112,114Sn

    R. Kumar, P. Doornenbal, A. Jhingan, R.K. Bhowmik, S. Appannababu, P. Bednarczyk, L. Caceres, J. Cederkall, A. Ekstrom, R. Garg, J. Gerl, M. Gorska, H. Grawe, J. Kaur, I. Kojouharov, S. Mandal, S. Mukherjee, S. Muralithar, W. Prokopowicz, P.P. Singh, P. Reiter, H. Schaffner, A. Sharma, R.P. Singh, D. Siwal, H.J Wollersheim, Act. Phys. Pol. B 42 (2011) 813..

  • Energy levels in 141Nd from fusion evaporation study

    S. Bhowal, C. Lahiri, R. Raut, P. Singh, M.K. Raju, A. Goswami, A.K. Singh, S. Bhattacharya, T. Bhattacharjee, G. Mukherjee, S. Bhattacharyya, S. Muralithar, R.K. Bhowmik, N. Madhavan, R.P. Singh, G. Gangopadhyay, J. Phys. (London) G 38 (2011) 035105..

View All

Contact us

Dr. S. Muralithar

Inter University Accelerator Centre Aruna Asaf Ali Marg, Post Box 10502 New Delhi 110067, India

Media Gallery

Back to Top