Experimental Condensed Matter Group
D. P. Mahapatra
B. N. Dev
S. N. Sahu
S. B. Ota
Shikha Varma
B. R. Sekhar
P. V. Satyam
T. Som
G. V. Raviprasad
D. P. Mahapatra
The microbeam facility of the IOP which was setup jointly
by IOP and SUNY at Albany is ready for routine use. Data have already been
taken on some samples involving self assembled island growths of metals
like Au, Ag etc on Si. Results are quite interesting and are going to be
presented in IBA-14/ECAART-6, Dresden, Germany. The spatial resolution
is about 5 microns where it is possible to get both x-ray and charged particle
spectra simultaneously.
On the AMS side the machine augmention is complete. The
new system has a 40 cathode MC-SNICS source along with a 450
spherical electrostatic analyser. The main idea behind using this analyser
is to reduce the high and the low energy tails in the sputter ion beam.
However, with rotatable electrodes it will also be used to inject beams
from our old alpha source for routine RBS,Channeling and PIXE works. The
injection magnet is replaced by a 900 double focussing injection
magnet with all the facilities for a fast isotope switching as may be necessary
for AMS work using 14C and 10Be beams. The high energy post acceleration
quadruple magnetic doublet lens has been replaced by a suitable electrostatic
quadruple triplet lens. Provision has been made to use an offset Faraday
cup for 13C(or 9Be) while carrying out 14C (or 10Be) measurements. A new
AMS beamline with a +150 cylindrical electrostatic analyser
has been erected along the -15deg line of the switching magnet. Last year
the new ionsource was erected as a standalone system with the 450
ESA and the 900 magnet in a different room and was thoroughly
tested. At the moment the MC source is operating at 35 kV only and the
transmission is not optimal.
Arrangements are being made to increase the injection
energy to about 50 keV where the transmission is expected to be good. The
computer control of the sequential injection of isotopes is being tested.
B. N. Dev
An energetic ion interacting with a solid loses energy
through electronic excitation in target atoms and scattering by target
atomic nuclei. If an energetic ion containing two atoms (dimer) enter into
a solid they can travel a short distance without being completely separated.
Within this distance in the solid, the closeness of the two components
of the dimer ion can cause modifications of the response of the electrons
in the solid, in comparison to the passage of monomer ions. We indirectly
observed this coherent dynamic response in C+2 implantation
into a semi-insulating GaAs crystal. In a semi-insulating material electronic
excitation can cause damage. We observed enhanced damage production in
the GaAs crystal surface region for C+2 implantation
compared to C+ implantation, where in both cases we used the
same energy/mass of the ions and the same atomic fluence. The near-surface
modified layer has been studied by X-ray reflectometry, Rutherford backscattering/
Channeling spectrometry and transmission electron microscopy. Transfer
of energy from the projectile ions to the atoms in the solid usually causes
damage to a crystalline solid. However, it can also bring order in a disordered
solid in a process like annealing. We have observed this phenomenon in
a grainy thin (~ 1000� epitaxial Ag(111) layer grown on a Br-passivated
Si(111) substrate. First we have demonstrated that it is possible to grow
an epitaxial Ag(111) layer under high vacuum conditions on a Br-passivated
Si(111) substrate. High resolution X-ray diffraction and ion channeling
experiments show that the Ag layer is epitaxial with (111) orientation.
However the crystalline quality is poor. Transmission electron microscopy
reveals that the layer is grainy instead of a continuous layer. Thermal
annealing upto 5000C improved the crystalline quality. This
happens through grain boundary melting and consequent growth of oriented
grains and the shrinkage of slightly misoriented grains. Exposure of the
Ag(111)/Si(111) sample to 1 MeV Si+ ion beam caused similar
effect as in thermal annealing. The displacement/ movement of Ag atoms,
having received energy from the incident Si+ ions, would be
dominant at the grain boundaries enhancing the growth of larger oriented
grains. This essentially improves the crystalline quality, which we quantitatively
measured by Rutherford backscattering and channeling experiments using
an MeV He+ ion beam.
A Si1-xGex alloy has an energy band
gap which is between the band gap values of Si and Ge. The band gap of
the alloy can be tuned by varying the comparison, x. This leads
to band gap engineering. If such a layer can be sandwiched between Si or
Ge, potential wells or barriers can be built within the material. Ion implantation
provides a way to prepare a buried sandwiched alloy layer. We have used
1 MeV Si+ implantation at an ion fluence of ~ 8.5 1017
cm-2 into a polised Ge(111) crystal to fabricate a buried Ge0.8Si0.2
layer. The actual composition varies somewhat depending on the post-implantation
annealing temperature. We studied the Si distribution in Ge, the implantation-induced
damage and recrystallization by Rutherford backscattering/ Channeling spectrometry
using MeV H+ and He+ ions.
S. N. Sahu
Nanocrystalline semiconductors with crystalline size comparable
to Bohr exciton radius show quantum size effect(SQE). For such semiconductors
showing QSE the continuum of energy levels broke down into discrete states
resulting widening of the band gap. The increased band gap show optical
properties far different from their bulk counter part. Apart from the deviation
in their optical properties these nanostructure semiconductors also exhibit
unusual structural,electrical,surface and intereface properties. In order
to confirm the above features, PbS and Porous Si nanocrystalline semiconductors
have been synthesized and their properties have been studied. PbS nanocrystalline
semiconductors have been grown by electrodeposition technique on conducting
substrates from precursers viz.PbSO4 and thiosulphate solution in acidic
media. Impurity and compositional analysis indicate stoicheometric deposits
and with out any impurities even at ppm level confirmed from RBS
and PIXE studies. RBS also predicted the surface roughness and measured
film thickness. Structural characterisation by XRD indicate a lattice distortion
of 1.5 %. Nanocrystalline sample surface show a branched fractal pattern.
Nanocrystalline PbS show QSE for size 18nm(estimated from AFM and XRD)
and a blue shift of 2.2 eV has been attained which is confirmed from optical
abosorption studies. Photoluminescence (PL) measurements show red shift
caused by structural diffects. PL measurements also show temperature insenistivity
of nanocrystalline sample indicate molecular nature of PbS.
Porous Si has ben synthesized by anodizing p-Si
in ethanol and HF mixture. The growth proces has been characterized by
in-situ Current (I)-Voltage (V) and Capacitance (C)- Voltage (V) measurements.
The in-situ C-V studies show two capacitance maxima corresponding to two
surface state energy levels generated by oxide growth. The contribution
of such surface states to capacitance at higher frequencies show to be
less dominant as expected. The in-situ I-V studies clearly identify the
pore formation, oxide growth and electro polishing regimes. These studies
are in progress.
The aging effect of uncapped nanocrystalline semiconductors
have been studied by photoluminescence measurements.For the above purpose
CdS nanocrystalline semiconductors have been grown by a chemical route
and stored for 15 and 30 days respectively and subjected to photoluminescence
measurements which has been installed in IOP recently. The PL studies show
that the crystalline size grows with time if not capped. The PL peaks are
red shifted and further shifted with aging suggests increase in crystalline
size.
S. B. Ota
We studied the magnetic properties of commercially available
cryogenic silicon diodes temperature sensors from CRYO Industries of America
Inc., in the temperature range 5-255K using a SQUID magnetometer. Further
analysis of the data was carried out. We conclude that the magnetic properties
of such diodes allow convenient background subtraction if used in close
proximity of the sample in magnetisation measurements.
Earlier we studied the forward characteristics of cryogenic
temperature sensor diodes. We concluded that such sensors can be used for
a range of current values with suitable calibration enhancing its applicability
as a low temperature sensor. A calorimeter is being constructed using such
a cryogenic temperature sensor diode. This setup is being built around
a Leybold closed cycle refrigerator. The computer program for automation
of the calorimeter setup has been developed. This computer program will
control the instruments using GPIB IEEE-488 interface. The software is
written using MS-DOS GWBASIC.
Further study of ergodicity of this technique for the
2d q- state Potts model was carried out. Ergodicity does not seem
to depend on the value of q. Lack of ergodicity, which occurs in
a particular situation, when the system energy is discrete as a function
of temperature is reported and discussed. This occurs only for small values
of system energy. This is a drawback especially when the system size is
small, as it limits the lowest temperature. However, such a situation does
not arise in models with continuous symmetry such as the XY-model.
It has been found that the temperature dependence of the
energy exhibits `S'-shaped nature at the first order transition of a finite
isolated system in microcanonical Monte Carlo simulations. Further study
was carried out on origin of `S'-shaped nature of the coexistence region
on the basis of the recently developed understanding. The present results
suggest independent study of finite size scaling of coexistence region
in microcanonical ensemble. In this context, we have estimated the interphase
surface entropy for the 2d Potts model and the extended 2d classical XY-model.
The 2d classical XY-model has been chosen as a model for
the real magnetic crystals. However, real magnetic crystals are subjected
to symmetry-breaking crystalline fields in addition to an isotropic exchange
coupling. In practice, we expect to encounter crystalline anisotropies
with 2-4 fold and 6-fold symmetries. However, a detailed
Monte Carlo study is lacking. Preliminary, microcanonical Monte Carlo simulations
have been carried out for the extended 2d XY-model undergoing first order
transition in the presence of a 3-fold symmetry-breaking field. It is observed
that the transition is clearly first order in nature and the coexistence
region of this first order transition is suppressed as the field strength
is increased. Preliminary computer simulations have been carried out on
the extended 3d classical XY-model undergoing first order transition.
Shikha Varma
Dose dependent structural modifications in Si(100) due
to 1.5~MeV implantation of Sb have been characterized using Raman spectroscopy
and Rutherford Backscattering Spectrometry/Channeling (RBS/C) techniques.
With increasing fluence, an intensity reduction of the 1st order
Raman peak, characteristic of crystalline Si, is observed. The amorphicity
in Si lattice appears at a dose of 1 1013 ions/cm2
and it increases with dose. For a dose of 5 1014 ions/cm2
the Raman spectrum resembles that of amorphous Si. RBS/C studies also support
a fully amorphized lattice at this dose though for smaller doses it suggests
lower disorder. For the fluences of 1 1013 ions/cm2
and 1 1014ions/cm2 a coexistence of undamaged
crystalline Si regions and amorphous zones is observed. Consequently phonon
confinement is observed. Lattice recovery achieved by subsequent annealing
has also been investigated using Raman Spectroscopy. By annealing at 6000C,
sample crystallinity is fully recovered in all the cases upto the fluence
of 5 1014 ions/cm2. For higher doses small
amorphicity still remains. Depth dependent measurements of the shifts in
the Raman peaks demonstrate a gradient in stress which is of compressive
nature near the surface region but is tensile in deeper layers. Maximum
stress in the lattice appears for a dose of 1 1012ions/cm2
which gets relaxed by the incorporation of amorphous zones at higher fluences.
We have also studied the density and nature of defects
produced in a sample with heavy high energy ions during implantation, using
IOP Pelletron . For this purpose we have carried out Channeling studies
of Sb implanted in Si and of Cu implantation in MgO. By removing the dechanneling
contributions, we have developed a Multiple Scattering Program or understanding
the modifications in density distribution during heavy ion implantations
as compared to TRIM model. For this investigation, Sb2+ ions
were implanted in Si(100) with a dose of 5 1015 ions/cm2
at IOP Pelletron. We investigated the spatial distribution of damage for
the implanted sample after annealing as well as after co-implantation with
8 MeV carbon (5 1016 atoms/cm2) ions at Room
Temperature(RT). Carbon irradiation resulted in an increase of sub-surface
damage. The increase in damage can be due to Sb and Si recoils produced
or due to mobile defects that drift from bulk towards the surface during
the carbon-irradiation. After annealing the irradiated sample to 8000C
a decrease in damage is observed. The spatial distribution of substitutional
fraction of Sb in Si has also been studied. In this regard we have also
made some SIMS measurements at IGCAR, Kalpakkam.
G. V. Raviprasad
Under the Accelerator Mass Spectrometry project, the existing
3MV tandem Van de Graaff pelletron accelerator will be augmented to do
radio carbon (14C) dating on the samples. We have developed
software to control the magnet power supplies for mass analysis and to
measure the beam currents through computer. We have successfully tested
the slow switching scheme where 13C and 14C beams
are alternately injected into the accelerator and their currents are measured
periodically every few seconds. The scheme was tested with 12C,
13C
and 12C, 16O systems with satisfactory results. A
new multi cathode SNICS source with a 45-deg electrostatic analyser has
been tested for fast switching through computer control and has been installed.
Trial runs are being taken to measure 14C/12C ratio.
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