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CHAPTER I: Bolometric detectors
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Figure 1.1: Spectral representation of investigated THz area [3] |
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Figure 1.2: a) Spectral density distribution of Planck’s blackbody
radiation, b) example of thermal imaging in the far infrared [7] |
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Figure 1.3:
Composite bolometric sensor with absorbing layer (η), bolometer resistive
body thermally connected to the heat sink at constant temperature T0. |
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Figure 1.4: R(T) characteristics of superconductor and
semiconductor bolometers |
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Figure 1.5: a) Interaction mechanism in a metallic bolometer
(normal bolometric effect) and b) in superconductor Hot Electron Bolometer
(HEB) |
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Figure 1.6: Frequency characteristic of YBaCuO superconductor thin
bolometer with normal bolometric area and with hot electron bolometric
response, calculated upon a three thermal reservoir flux model [10] |
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Figure 1.7: a) NbN nanobolometer with log-periodic spiral antenna
[14], b) detail of such a nanobolometer patterned in an ultra-thin
superconductor Nb film [15] |
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Figure 1.8: Translation of frequency spectrum in heterodyne
detection |
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Figure.
1.9: Heterodyne
detection on a resistive bolometer body
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CHAPTER II: MOS
Transistor
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Figure 2.1: a) Simple N-channel type transistor MOS with the
substrate (bulk), drain, gate and source electrodes and thin insulating
SiO2 barrier b) schematic symbols of N and P-MOS transistors |
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Figure 2.1: a) Simple N-channel type transistor MOS with the substrate
(bulk), drain, gate and source electrodes and thin insulating SiO2
barrier b) schematic symbols of N and P-MOS transistors |
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Figure 2.2: Cross-section of planar N-MOS and P-MOS transistor in
common P-type substrate, with indicated parasitic thyristor causing the
latch-up effect |
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Figure 2.3: Cross-section e of a six-level metallic connection
[38] |
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Figure 2.4: Idealized MOS capacitor demonstrating the charge
distribution dependence on the Gate-to-Bulk voltage VGB. The
gate is composed from the isolated elements of the voltage increasing
along the channel (this is not real MOS device!) |
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Figure 2.5: N-Channel transistor MOS with induced channel, allowing
the current transfer between the drain and source |
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Figure 2.6: N-Channel MOS transistor in saturation with a) VDS=VGS –VTH:
dashed line and b) VDS > VGS – VTH : dark
area |
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Figure 2.7: Measured characteristic of N-MOS transistor 15/5 µm a)
ID vs. VGS with plotted gm = dID/dVGS
b) ID vs. VGS characteristic for the same transistor
for various VGS voltage |
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Figure 2.8:
Effect of channel length modulation to the current I |
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Figure 2.9: Static small signal model of the MOS transistor
containing the gate and substrate transconductance gm an gB,
and channel resistance rDS (=1/gDS) |
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Figure 2.10: a) MOS terminal capacitances, b) physical
interpretation off the MOS capacitances |
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Figure 2.10: b) physical interpretation off the MOS capacitances |
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Figure 2.11: C-V characteristic of the N-MOS 15 µm/5 µm
transistor.(Terminals D, S, B are grounded) |
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Figure 2.12: C-V characteristic of gate capacitance plotted as
function of VGS and VDS showing the transition
between the ohmic and saturation area (N-MOS 15µm/5µm) |
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Figure 2.13: AC small signal model of the MOS transistor |
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Figure 2.14: AC small signal model without substrate effect |
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Figure 2.15: I-V characteristic of transistor in linear, saturated
and velocity saturated regions (plotted for N-MOS 10 µm/1 µm) |
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Figure 2.16: gm/ID characteristic of an N-MOS
and P-MOS AMS 0.35µm transistor drawn from Spice-level 7 model |
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Figure 2.17: Cross section
of the AMS 0.35µm process |
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Figure 2.18: 45nm Intel TriGate transistor, a) AFM image; b)
schematic design
[34] |
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Figure 2.18: 45nm Intel TriGate transistor, a) AFM image; b)
schematic design
[34] |
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Figure 2.19: Single Electron Transistor (SET) a) structure with two
tunnel junctions,
b) drain current periodicity with island charge
[36] |
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Figure 2.19: Single Electron Transistor (SET),
b) drain current periodicity with island charge
[36] |
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CHAPTER III: Noise
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Figure 3.1: Generated sequence of noise with Gaussian distribution
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Figure 3.2: Demonstration of noise power transfer between two
resistors maintained at different temperatures |
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Figure 3.3: Power spectral density (PSD) of generated white and 1/f
noise sequences |
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Figure 3.4: Construction of an equivalent input noise voltage
source |
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Figure 3.5:
Equivalent input noise voltage of bipolar transistor as a function of
input resistance RS |
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Figure 3.6: Simplified small signal noise model of the MOS
transistor |
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Figure 3.7: a) Feedback-free and b) feedback configuration of
amplifiers with noise source modelling the noise of input amplifier stage |
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Figure 3.8: Chopper (auto zero) amplifier reducing the 1/f noise |
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Figure 3.9:
Josephson junction composed of two superconducting electrodes and weak
insulator link |
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Figure
3.11: a) DC SQUID realized with two
Josephson junction, b) schematic design with an external coupling
inductance
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| Chapter
IV-X : in preparation |