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laboratory is equipped with a complete thermal
analysis system from Shimadzu. The system includes
(from right to left below) a DTA50 differential
thermal analyzer with a 1600 °C temperature
maximum, a TGA50 thermogravimetric analyzer with
a 1600 °C temperature maximum and a DSC60
differential scanning calorimeter with a 600 °C
temperature maximum.

These
three instruments run off the same TA60WS controller
and can be operated simultaneously. There is also
a FC-60A gas flow controller for experiments to
be done under N2, Argon or O2
atmosphere. These three complimentary techniques
allow us to study melting points, decompositions,
phase transitions, glass transitions and weight
losses as a function of temperature under various
atmospheres. This information helps us design
our synthetic experiments to best prepare the
new materials in pure form and to design crystal
growth experiments.
A new MBraun LabMaster 130 double glove box with
a single filter column gas purification system
shown below is used for the manipulation of air-sensitive
and moisture-sensitive products and starting materials.
The glovebox is equipped with a CCD camera, Optem
1:10 zoom, with a color video monitor. With the
use of a switch box the image can be transferred
from the video monitor over to a PC where it can
be saved for future reference or printed out for
pasting into laboratory notebooks.

Our Cary5000 UV/Vis/NIR spectrometer from Varian
(shown below) is used to study the optical properties
of our new materials. From diffuse reflectance
measurements we estimate the band gap energies
of our new semiconductor compounds.

For diffuse reflectance we use the Praying Mantis
attachment from Harrick Scientific (shown below).
 
It
incorporates two 6:1, 90° off-axis ellipsoids,
which form a highly efficient, diffuse reflection
illumination and collection system. This unique
configuration deflects the specular reflectance
away from the collecting ellipsoid, minimizing
the associated spectral distortions. This attachment
is also used with a rear beam attenuator. We also
have an ambient sample chamber to go inside the
praying mantis. This chamber allow us to prepare
our air-sensitive materials for measurement inside
our glovebox, seal them up in the chamber, and
bring them out of the box to take measurements.
The praying mantis is better than an integrating
sphere for our work. One reason is because you
can use much less sample and you can recover the
sample after the measurement. Another reason is
that it is not wavelength limiting. The Praying
Mantis allows us access to the entire UV/Vis/NIR
range. We can also pop the attachment out of the
Cary 5000 and insert it into almost any FT-IR
instrument. For measurements in the mid-IR range
we are using the new Nexus 470 FT-IR by Thermo
in the lab of Dr. Ellen Gawalt down the hall.
Most of our reactions are carried out in sealed
tubes under vacuum. The tubes are made of either
Pyrex or Fused-Silica depending on the reaction
temperature used. We use a Natural gas/O2
flame to make the reactions tubes. The tubes are
loaded with the solid reactants in the inert atmosphere
glovebox under Argon. The tubes are then removed
from the box and attached to this high vacuum
line, shown below. The line is evacuated by an
Edwards pumping system, which consists of an RV5
backing pump and an E050/60 air-cooled diffusion
pump. An Edwards wide range gauge reads from atmospheric
pressures all the way down to 5 x 10-9
mbar. In most cases we can usually get the line
to pump down into the 10-5 range.

We have a Precision Thelco mechanical convection
oven (below) with a maximum temperature of 250°
C. It is controlled by a microprocessor temperature
control so that no one needs to be in the lab
to shut it off when a reaction is finished.

We
also have a Venticell oven by Grieve (left below)
for the same purpose. These ovens are used for
the heating of our solvothermal reactions. Each
reaction is contained in PTFE cup, which is inserted
into a Parr 23 ml acid digestion bomb. A Scientific
Products vacuum oven (right below) with a maximum
temperature of 225° C is used to dry samples
under vacuum. Samples that are dried under vacuum
are usually those obtained via solution chemistry.
The oven is evacuated by an Edwards RV3 vacuum
pump and is capable of holding a vacuum of 30
inches of Hg.

What
is a solid-state inorganic lab without high-temperature
furnaces? We currently have four hinged tube furnaces
in our laboratory. The three minimites by Lindberg
have a maximum temperature of 1100 °C and
can fit about 4 reactions tubes per run (shown
on the right below). A large Thermolyne furnace
has a maximum temperature of 1200 °C and can
fit up to 20 reactions at once (left below). We
also have the use of a furnace capable of reaching
1700 °C over in the lab of our collaborator,
Monica Sorescu, in the Physics Department at Duquesne.

We are currently in the process of designing our
own furnaces, which we will assemble next year
with the help of our competent instrument shop
personnel who are specialists in the area of electronics.
Our supply of Pyrex and Fused-Silica used to make
reaction tubes is stored in this professional
glassblowers supply cabinet. The cabinet is nearly
full with several different sizes of tubing including
8mm, 9mm, 11mm and 12 mm OD. We have several different
sized Swagelock adapters to attach these sizes
of tubing to the high-vacuum line.

The
larger of our two laboratories has been completely
renovated (see photo below) with new casework
and a new fume hood. The smaller laboratory is
equipped with two more fume hoods.

Powder
X-ray diffraction measurements are performed on
our Rigaku DmaxB powder X-ray diffractometer using
Cu Ka radiation. An automatic sample changer allows
us to do up to 25 samples in sequence. The instrument
is located in the Bayer Learning Center and is
available free of charge to all researchers at
Duquesne University.

Currently
single crystal X-ray diffraction experiments are
performed on our Rigaku AFC7R rotating anode X-ray
diffractometer that is equipped a Mo Ka radiation.

Recently
our department has been awarded an NSF-CRIF grant
to obtain a new diffractometer with a CCD area
detector. The instrument will be used first and
foremost for elucidation of new crystal structures
involved in Duquesne University research projects;
however, it will be also used as tool for teaching
X-ray crystallography. Several area colleges have
expressed interest in becoming involved with our
"teaching and learning center for X-ray diffraction".
We hope to provide remote access to the instrumentation
so that students from other universities can collect
data on their samples without actually traveling
to Duquesne University. In addition, we hope to
get more Duquesne students interested in X-ray
diffraction by developing a skills course in X-ray
diffraction techniques.
Magnetic measurements are performed in the laboratory
of our collaborator, Monica Sorescu, using a susceptometer-magnetometer
system with a 3 Tesla superconducting magnet and
liquid helium cryostat for dc hysteresis loops
and ac susceptibility measurements (shown below).
We are using this measurement system to study
our diluted magnetic semiconductors based on diamond-like
semiconductors.

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