The document announces open houses at the Materials Characterization Lab to showcase various characterization techniques. It provides dates and times for demonstrations of techniques like thermal analysis, electron microscopy, X-ray diffraction, and dielectric characterization. The open houses will take place between June and August at various campus locations, including the MRL and MRI buildings.
Semiconductor lasers are ideally suited for mass production and widespread applications, because they are based on a wafer-scale technology with a high level of integration. Not surprisingly, the first lasers entering virtually every household were semiconductor lasers in compact disk players. A new ultrafast semiconductor laser concept has been introduced by Prof. Keller, which is power scalable, suitable for pulse repetition rate scaling in the 10 to 100 GHz regime, supports both optical and electrical pumping and allows for wafer-scale fabrication. This class of devices is referred to as the modelocked integrated external-cavity surface emitting laser (MIXSEL). The next step towards even lower-cost and more compact ultrafast lasers will be electrical pumping with both pico- and femtosecond pulses. This would result in devices ideally suited for many applications such as telecommunications, optical clocking, frequency metrology, high resolution nonlinear multiphoton microscopy, optical coherence tomography, laser display . anywhere where the current ultrafast laser technology is considered to be too bulky or expensive.
The project aims to demonstrate optically and electrically pumped MIXSELs in both the pico- and femtosecond regime. Picosecond MIXSELs are ideally suited for clocking applications whereas femtosecond MIXSELs are required for continuum generation and many biomedical applications. For both cases, average powers above 100 mW with electrical pumping and above 500 mW with optical pumping should be reached, which represent significant advances of ultrafast MIXSELs.
Semiconductor lasers are ideally suited for mass production and widespread applications, because they are based on a wafer-scale technology with a high level of integration. Not surprisingly, the first lasers entering virtually every household were semiconductor lasers in compact disk players. A new ultrafast semiconductor laser concept has been introduced by Prof. Keller, which is power scalable, suitable for pulse repetition rate scaling in the 10 to 100 GHz regime, supports both optical and electrical pumping and allows for wafer-scale fabrication. This class of devices is referred to as the modelocked integrated external-cavity surface emitting laser (MIXSEL). The next step towards even lower-cost and more compact ultrafast lasers will be electrical pumping with both pico- and femtosecond pulses. This would result in devices ideally suited for many applications such as telecommunications, optical clocking, frequency metrology, high resolution nonlinear multiphoton microscopy, optical coherence tomography, laser display . anywhere where the current ultrafast laser technology is considered to be too bulky or expensive.
The project aims to demonstrate optically and electrically pumped MIXSELs in both the pico- and femtosecond regime. Picosecond MIXSELs are ideally suited for clocking applications whereas femtosecond MIXSELs are required for continuum generation and many biomedical applications. For both cases, average powers above 100 mW with electrical pumping and above 500 mW with optical pumping should be reached, which represent significant advances of ultrafast MIXSELs.
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Dielectric
1. Materials Characterization Lab
www.mri.psu.edu/mcl
Dielectric Characterization
Paul Moses
paulmoses@psu.edu
167 MRL
814-863-0857
June 6, 2005
2. Materials Characterization Lab
www.mri.psu.edu/mcl
Summer Characterization Open Houses
Technique Time Date Location
Thermal analysis (TGA, DTA, DSC) 9:45 AM June 8 250 MRL Bldg.
Transmission Electron Microscopy (TEM/STEM) 9:45 AM June 15 114 MRI Bldg
Scanning electron microscopy (SEM) 9:45 AM June 22 541 Deike Bldg.
Analytical SEM 11:00 AM June 22 541 Deike Bldg.
X-ray Diffraction (XRD) 9:45 AM June 29 250 MRL Bldg.
Dielectric Characterization (25 min lecture only) 9:45 AM July 6 250 MRL bldg.
High temperature sintering lab (20 min lecture only) 10:15 AM July 6 250 MRL Bldg.
Focused Ion Beam (FIB) 9:45 AM July 13 114 MRI Bldg
TEM sample preparation 11:00 AM July 13 114 MRI Bldg
Orientation imaging microscopy (OIM/EBSD) 9:45 AM July 20 250 MRL Bldg.
Chemical analysis (ICP, ICP-MS) 9:45 AM July 27 541 Deike Bldg.
Atomic Force Microscopy (AFM) 9:45 AM August 3 114 MRI Bldg
Small angle x-ray scattering (SAXS) 9:45 AM August 10 541 Deike Bldg.
Particle Characterization 9:45 AM August 17 250 MRL
X-ray photoelectron spectroscopy (XPS/ESCA) 9:45 AM August 24 114 MRI Bldg
Auger Electron Spectroscopy (AES) 11:00 AM August 24 114 MRI Bldg
NOTE LOCATIONS: The MRI Bldg is in the Innovation Park near the Penn Stater Hotel; MRL Bldg. is on Hastings Road.
More information: www.mri.psu.edu/mcl
3. Materials Characterization Lab
Materials Characterization Lab Locations www.mri.psu.edu/mcl
Bldg Telephone
MRL 863-7844
MRI 865-0337 MRI Bldg:
Hosler 865-1981
XPS/ESCA, SIMS,
E&ES 863-4225
TEM, HR-TEM, FE-
Auger, AFM, XRD
MRL Bldg:
Hosler Bldg:
SEM, XRD, OIM, DTA,
SEM, ESEM, FE-
DSC, TGA, FTIR, Penn Stater
SEM, EPMA, ICP,
Raman, AFM, Powder, Hotel
E&ES Bldg: ICP-MS,BET, SAXS
dielectric, prep, shop,
SEM
IC, UV-Vis
Route 322
Steidle Bldg:
Nanoindenter
Atherton Street
(322 Business)
I-99
0
Park
0 0
0 0 0 0
0
Ave.
0 0 0 0
Park 0
0
Beaver
A0ve. Stadium
0
0
0
Centre
0
0
Community
Porter Road
Univ
Shortlidg
Hospital
0
0
Burrowes Road
ersi
ty D
e Road
Pollock Road
rive
North
Hastin
Deike Bldg: Road gs
College Ave.
5. Materials Characterization Lab
www.mri.psu.edu/mcl
What's Dielectric Characterization?
E.G.: conductivity (V=RI), permittivity (D= E), impedance (V*=Z*ยทI*),
piezoelectricity (P=dฯ), pyroelectricity (i=pยทdT/dt), ferroelectricity (nonlinear
relationship between electric field, polarization, strain, ...)
For sure it involves charge and many orders of magnitude.
6. Materials Characterization Lab
www.mri.psu.edu/mcl
Irreversible (DC) Reversible (AC)
V = RI
LCR Meter
PE
D33 Meter
Quasi-Static Strain
Charge/Analyzer
Pulse Discharge
RF IV
IV
Others including transformer ratio bridges, microwave
techniques, ๏ฌuid immersion
7. Materials Characterization Lab
www.mri.psu.edu/mcl
Irreversible (DC)
Pulse
PE CV
Discharge
4
0 9
9
-3
-3 0 3 6 -3 0 3 69
-3 0 3 6
V V V
I
I
8. Materials Characterization Lab
www.mri.psu.edu/mcl
Reversible (AC)
Charge Converter
LCR RF IV
Network Analyzer
Meter
4
0
-3
-3 0 3 69 -3 0 3 69 -3 0 3 69
V
Ref
V
V
Test
I
9. Materials Characterization Lab
www.mri.psu.edu/mcl
PE LCR Charge RF-IV
CV
Pulse LCR++ Charge++ RF-IV++
4
Log Voltage
0
-3
-3 0 3 6 9
Log Frequency
10. Materials Characterization Lab
www.mri.psu.edu/mcl
How To Get Started
contact: Jeff Long or Paul Moses
you will need:
โ a question or a plan
โ a sample with electrodes, contacts, or connections
โ a budget/fund number (cost center/project number)
โ possibly expendables: silver foil, dielectric fluid
โ possibly special fixture