Tehnici nanolitografice pentru fabricarea dispozitivelor ... - ICPE-CA
Tehnici nanolitografice pentru fabricarea dispozitivelor ... - ICPE-CA
Tehnici nanolitografice pentru fabricarea dispozitivelor ... - ICPE-CA
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12 October 2012<br />
<strong>Tehnici</strong> <strong>nanolitografice</strong> <strong>pentru</strong> <strong>fabricarea</strong><br />
<strong>dispozitivelor</strong> nanoelectronice<br />
Adrian Dinescu, IMT Bucuresti<br />
Workshop “Parteneriat <strong>pentru</strong> inovare: cercetare – industria electronica”
18 October 2012<br />
Nanoscale Structuring and Characterization Laboratory<br />
Raith e_Line - dedicated EBL equipment NanoInk Nscriptor – dip pen nanolithography<br />
Tescan Vega LMU II<br />
Thermionic (tungsten) SEM<br />
FEI Nova NanoSEM630<br />
FEG-SEM<br />
NT-MDT Ntegra Aura AFM & STM<br />
Agilent G200 - Nanoindenter
First EBL equipment in IMT - Tescan Vega LMU II<br />
and Raith Elphy Plus – installation 2006 Raith e-Line – installation 2008<br />
18 October 2012<br />
Smallest beam diameter : 5nm @ 3pA<br />
beam current and 30kV<br />
100nm<br />
Electron Beam Lithography equipment in IMT Bucharest<br />
30nm diameter holes in PMMA 950k<br />
Smallest beam diameter: 1.5nm @ 200pA<br />
150nm<br />
̴ 10nm diameter holes in PMMA 950k
600µm<br />
18 October 2012<br />
Mix and match lithography: photolitography & EBL<br />
200µm
18 October 2012<br />
Acoustic devices for GHz applications<br />
Acoustic resonators<br />
A.Muller, D. Neculoiu, G. Constantinidis, G. Deligeorgis, A. Dinescu, A. Stavrinidis, A. Cismaru, M. Dragoman and A. Stefanescu,<br />
„ SAW Devices manufactured on GaN/Si for frequencies beyond 5GHz”, IEEE Electron Device Letters, Vol. 31, No. 12, Dec. 2010<br />
D. Neculoiu, A. Müller, G. Deligeorgis, A. Dinescu, A. Stavrinidis, D. Vasilache, A. Cismaru, G. E. Stan and G. Konstantinidis,<br />
“AlN on silicon based surface acoustic wave resonators operating at 5 GHz”, Electronics Letters, vol 45, No 23, 2009
18 October 2012<br />
AlN/Si<br />
•Deposition by magnetron sputtering<br />
•Sound velocity 6000 m/s<br />
•Coupling coefficient ̴ 6%<br />
GaN/Si<br />
•Deposition by MBE and MOCVD<br />
•Sound velocity 5000 m/s<br />
•Coupling coefficient ̴ 2%<br />
•Monolithic integration with HEMT<br />
transistors is possible<br />
SAW devices for microwave applications (1)<br />
HEMTs<br />
SAWs<br />
Collaboration IMT Bucharest – FORTH IESL Heraklion, Grece
GDSII layout for contact<br />
pads and alignment marks<br />
18 October 2012<br />
Detail of Ti/Au<br />
nanoelectrodes<br />
SAW devices for microwave applications (2)<br />
Photolithography<br />
Metallization<br />
(Cr/Au)<br />
Lift off<br />
Wafer patterned with Cr/Au<br />
contact pads<br />
SAW resonator after<br />
metallization and lift off<br />
+<br />
E-beam evaporation<br />
(Ti/Au)<br />
Lift off<br />
GDSII layout of the IDTs<br />
EBL<br />
IDTs patterned in PMMA 950k
SAW devices for microwave applications (5)<br />
Results 2009<br />
Resonance > 5GHz on AlN<br />
D. Neculoiu, A. Müller, G. Deligeorgis, A. Dinescu, A.<br />
Stavrinidis, D. Vasilache, A. Cismaru, G. E. Stan and G.<br />
Konstantinidis, “AlN on silicon based Surface Acoustic<br />
Wave resonators operating at 5 GHz”<br />
-70<br />
4.6 4.8 5<br />
frequency, GHz<br />
5.2 5.4<br />
Electron. Lett. 45, 1196 (2009) Best previous result obtained before was a SAW on<br />
AlN (but on diamond not on silicon) operating at 4.5<br />
GHz [P. Kirsch et al. Appl Phys. Lett.88, 223504,<br />
2006]<br />
18 October 2012<br />
S21, dB<br />
-40<br />
-45<br />
-50<br />
-55<br />
-60<br />
-65
18 October 2012<br />
SAW devices for microwave applications (6)<br />
SEM micrograph of the test structure. The distance between the IDTs was d = 20 µm;<br />
for the other test structures, it was d = 100, 200, and 600 µm.<br />
Detail of the nanolithographic process with fingers and interdigits which are<br />
nominally 200-nm wide, developed on the GaN surface.<br />
(a) SEM photograph. (b) AFM image.<br />
A.Muller; D.Neculoiu; G.Konstantinidis; G. Deligeorgis; A. Dinescu; A.<br />
Stavrinidis; A. Cismaru; M.Dragoman; A.Stefanescu; “SAW Devices<br />
Manufactured on GaN/Si for Frequencies Beyond 5 GHz “<br />
IEEE ELECTRON DEVICE LETTERS Volume: 31 Issue: 12 Pages:<br />
1398-1400 1398 1400 (2010)<br />
Results 2010<br />
Resonance > 5GHz on GaN<br />
Measured reflection losses (S11) versus the frequency for three<br />
structures with different distances between the IDTs compared<br />
with the electromagnetic simulated results (without the<br />
inclusion of the piezoelectric effect).<br />
The highest resonance frequency reported for a SAW structure on GaN (on sapphire) is<br />
2.225 GHz, with the interdigitated transducer (IDT) having 600-nm-wide fingers and<br />
spacings: T. Palacios, F. Calle, E. Monroy, and F. Munoz, “Submicron technologyfor IIInitride<br />
semiconductors,” J. Vac. Sci. Technol. B, Microelectron. Process. Phenom., vol.<br />
20, no. 5, pp. 2071–2074, Sep. 2002.
SAW, single resonator; length 100 µm<br />
IDTs, digit/interdigit spacing 0.2 µm;<br />
Distance between reflectors and IDTs:<br />
d= 0.95 µm;<br />
IDT: 100 fingers/interdigits ; reflectors<br />
60 digits /interdigits<br />
GaN/Si; GaN layer 1 µm thin<br />
IDT and reflectors 0.1 µm thin Au<br />
18 October 2012<br />
SAW devices for microwave applications (7)<br />
SmartPower - Smart integration of GaN & SiC high power electronics for industrial<br />
and RF applications. (www.smart-power.com)<br />
Experiments to prove the concept of monolithic integration of MMIC and GaN T sensor.<br />
Q = 400<br />
Sensitivity ~ 356.9 kHz/°C<br />
= 65 ppm/°C
18 October 2012<br />
MSM photodetectors on silicon supported GaN membranes<br />
Schematic cross-section of the membrane<br />
MSM UV detector structure.<br />
Top view of the detector Detail of the interdigitated contacts<br />
a) Responsivity vs wavelength for the 0.5µm finger/interdigit UV GaN detector before the silicon substrate removal.<br />
b) Responsivity vs wavelengthfor the 0.5 µm finger/interdigit UV detectorst manufactured on thin GaN membrane.<br />
1. A.Muller, G. Konstantinidis, M. Dragoman, D. Neculoiu, A. Dinescu, M. Androulidaki, M. Kayambaki, A. Stavrinidis, D. Vasilache, C. Buiculescu, I. Petrini, A. Kostopoulos and<br />
D. Dascalu, “GaN Membrane-supported UV Photodetector manufactured using nanolithographic process” , Microelectronics Journal; ,40,2009, p 319-321.<br />
2. A. Müller, G. Konstantinidis, M. Androulidaki, A. Dinescu, A. Stefanescu , A. Cismaru , D. Neculoiu , E. Pavelescu, A. Stavrinidis, “Front and backside-illuminated GaN/Si<br />
based metal–semiconductor–metal ultraviolet photodetectors manufactured using micromachining and nano-lithographic technologies”, Thin Solid Films, 520 (2012)<br />
2158–2161
Schematic cross-section of the membrane<br />
MSM UV detector structure.<br />
18 October 2012<br />
MSM photodetectors on silicon<br />
E. Budianu, M. Purica, A. Dinescu, E. Manea “Metal-Semiconductor-Metal photodetector on silicon insulating wafers<br />
based on nanoscale interdigitated electrodes”, EMRS Fall meeting 2009, September 14-18, Warsaw, Poland
18 October 2012<br />
AFM image of the SLG<br />
Equipment: NT-MDT N-Tegra Aura<br />
Intensity (a. u.)<br />
1581.0<br />
EBL for graphene based devices<br />
2656.7<br />
1 500 2 000 2 500 3 000 3 500 4 000<br />
Raman shift (cm -1 )<br />
Intensity (a. u.)<br />
1583.2<br />
A.C. Ferrari et. al., Pyhs. Rev. Lett. 97 , 187401 (2006)<br />
MLG BLG SLG<br />
2657.6<br />
1 500 2 000 2 500 3 000 3 500 4 000<br />
Raman shift (cm -1 )<br />
Intensity (a. u.)<br />
1586.1<br />
2640.7<br />
1 500 2 000 2 500 3 000 3 500 4 000<br />
Raman shift (cm -1 )<br />
Raman spectra of a few selected points of graphene flake used for FET fabrication<br />
Substrate: p ++ silicon, boron doped, resistivity 0.005 Ωcm, covered with 300nm dry thermal oxide
18 October 2012<br />
SLG areas surrounded by alignment marks
18 October 2012<br />
Patterned electrical contacts on graphene flakes
18 October 2012<br />
CPW structures on SLG
18 October 2012<br />
Cutting process for<br />
SLG<br />
- Electronresist<br />
-SLG<br />
-Silicon dioxide<br />
-Silicon<br />
Electron resist deposition<br />
EBL exposure<br />
RIE (oxygen plasma)<br />
Electron resist removal<br />
E-beam lithography patterning of graphene flake<br />
RIE etching (oxygen plasma) of graphene flake
18 October 2012<br />
Intensity (a. u.)<br />
1588.1<br />
2642.8<br />
1 500 2 000 2 500 3 000 3 500 4 000<br />
Raman shift (cm -1 )<br />
Electrical contacts for source and drain fabricated by e-beam lithography, metal<br />
evaporation (Ti/Au- 5-30nm), and lift-off
18 October 2012<br />
Pristine SLG<br />
Graphene patterned for RIE<br />
Patterning in the PMMA before metal coating The structre with 20 transistors after lift-off<br />
Array of 17 back gated FETs on graphene ribbons<br />
Graphene ribbons<br />
A back gated FET on<br />
graphene ribbon
Rds (kΩ)<br />
Semiconductor Characterization System - 4200-SCS/C/Keithley<br />
with Wafer Probing Station –Easyprobe EP6/ Suss MicroTec<br />
18 October 2012<br />
14<br />
12<br />
10<br />
8<br />
6<br />
4<br />
2<br />
0<br />
-40 -30 -20 -10 0 10 20 30 40<br />
Back gate voltage (V)<br />
R d s i n th e C N P (k Ω )<br />
80<br />
70<br />
60<br />
50<br />
40<br />
30<br />
20<br />
10<br />
The device under test, on the probing station<br />
0<br />
0 200 400 600 800 1000 1200<br />
Dose (µC/cm2)<br />
Rds in the CNP vs irradiation dose (HV = 200V)<br />
Similar behavior at 500V and 1kV
18 October 2012<br />
EBID module<br />
SEM micrographs showing platinum lines connecting a polymer nanowire to the electrical pads<br />
L. Gence, V. Callegari, A Dinescu, S. Melinte and S. Demoustier-Champagne, “Hybrid Polymer nanowire based electronic devices correlated characterization”<br />
14-th International Conference of Modulated Semiconductor Structures (MSS 14), 19-24 July 2009, Kobe, Japan
• Project: Carbon nAnotube Technology for High-speed nExt-geneRation nano-<br />
InterconNEcts – <strong>CA</strong>THERINE (FP7/STREP, 2008-2010)<br />
Structure used for electrical characterization of CNTs<br />
at high frequencies. EBL was used for patterning the<br />
small calibration line and EBID technique for fixing<br />
the CNTs<br />
18 October 2012<br />
Platinum deposition was used for fixing the CNTs<br />
across V-shaped trenches in order to measure their<br />
mechanical properties