terahertz spectroscopy and applications frank c. de lucia department of physics

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Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics Ohio State University IEEE International Frequency Control Symposium June 5 - 7, 2006 Miami, Florida

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Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics Ohio State University IEEE International Frequency Control Symposium June 5 - 7, 2006 Miami, Florida. PEOPLE Doug Petkie - Professor WSU Eric Herbst - Professor OSU Brenda Winnewisser - Adj. Professor OSU - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Terahertz Spectroscopy and Applications

Frank C. De LuciaDepartment of PhysicsOhio State University

IEEE International Frequency Control SymposiumJune 5 - 7, 2006 Miami, Florida

Page 2: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

PEOPLE

Doug Petkie - Professor WSUEric Herbst - Professor OSU

Brenda Winnewisser - Adj. Professor OSUManfred Winnewisser - Adj. Professor OSU

Paul Helminger - Professor USAAtsuko Maeda - Research AssociateIvan Medvedev - Research AssociateAndrei Meshkov - Graduate StudentTJ Ronningen - Graduate Student

Laszlo Sarkozy - Graduate StudentDavid Graff - Graduate StudentCory Casto - Graduate Student

Kerra Fletcher - Graduate StudentBryan Hern - Undergraduate Student

Drew Steigerwald - Undergraduate StudentJohn Hoftiezer - Electrical Engineer

Page 3: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

The Lay of the Land

What is the basic physics of the SMM/THz?

How does this impact technology and frequency control?

What physics does it lead us to naturally - What are the important applications?

Where is the excitement?

Page 4: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

What is the Physics of the SMM/THz? The Energetics: h ≤ kT

The Classical Size Scale ≤ 1 mm

Noise

Interactions: Gases, Liquids, and Solids

Atmospheric Absorption

Classical Scattering and Penetration

Page 5: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Technology and Frequency Control

Solid-State THz Sources (CW)

0.001

0.01

0.1

1

10

100

1000

10000

10 100 1,000 10,000 100,000

Frequency (GHz)

Po

wer

(mW

)

Page 6: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

What are the Field Applications?

Orion. IRAM 30-m telescope line survey

Atmospheric Chemistry

Astrophysics

Page 7: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Where is the New Excitement?

4 0 0

3 0 0

2 0 0

1 0 0

0

- 1 0 0

3 3 3 .1 03 3 3 .0 83 3 3 .0 63 3 3 .0 43 3 3 .0 23 3 3 .0 0x 1 0

3

3 0 0 0

2 0 0 0

1 0 0 0

0

- 1 0 0 0

3 7 0 x 1 03

3 6 03 5 03 4 03 3 0F re q u e n c y ( M H z )

4 0 0

2 0 0

0

-2 0 0

3 3 3 .1 0 x1 03

3 3 3 .0 83 3 3 .0 63 3 3 .0 43 3 3 .0 23 3 3 .0 0Frequency (MHz)

#09 Acrylontrile Library

Combined Spectrum

Medical

New Physical RegimesAnalytical Applications

Active and Passive Imaging

Page 8: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Temperature

kT (300 K) = 200 cm-1

kT (1.5 K) = 1 cm-1

kT (0.001 K) = 0.0007 cm-1

Fields

qE (electron) >> 100000 cm-1

mE (1 D) ~ 1 cm-1

mB (electronic) ~ 1 cm-1

mB (nuclear) ~ 0.001 cm-1

The THz has defined itself broadly and spans kT

The Physics - The EnergeticsAtoms and Molecules

E (electronic) ~ 50000 cm-1

E (vibrational) ~ 1000 cm-1

E (rotational) ~ 10 cm-1

E (fine structure) ~ 0.01 cm-1

Radiation

UV/Vis > 3000 cm-1

IR 300 - 3000 cm-1

FIR 30 - 300 cm-1

THz 3 - 300 cm-1

MW 1 - 10 cm-1

RF < 1 cm-1

Page 9: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

The ‘Gap’ in the Electromagnetic Spectrum

Solid-State THz Sources (CW)

0.001

0.01

0.1

1

10

100

1000

10000

10 100 1,000 10,000 100,000

Frequency (GHz)

Po

wer

(mW

)

[From Tom Crowe UVA/VDI]

Size

h/kT

Cooling

Tubes, a little more - Photomixers, a little less

Page 10: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

PN ~ kT (Bmax )1

2 ~ kTmax

B

max

12

Blackbody Brightness [W/cm2-Hz]

Thermal Noise and Power in the THz

From E. Brown

Number of modes/cm2 ~ 1/(cm)

Blackbody Noise/mode

Thermal Noise below cutoff frequency max in integration bandwidth B

Thermal noise in bandwidth b with integration bandwidth B

PN kTb

PN kT (bB)1/2

Page 11: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

The THz is VERY Quiet even for CW Systems in Harsh Environments

QuickTime™ and a Photo - JPEG decompressor are needed to see this picture.

Experiment: SiO vapor at ~1700 K

All noise from 1.6 K detector system

1 mW/MHz -> 1014 K

1mW/100 Hz -> 1018 K

“Noise, detectors, and submillimeter-terahertz system performance in nonambient environments”

Frank C. De Lucia

J. Opt. Soc. B, 1275 (2004)

Page 12: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

What is the Physics of Interactions?

Separate into Three Classes by Linewidth

Low pressure gases: Q ~ 106

Atmospheric pressure gases: Q ~ 102

Solids and Liquids: Q ~ 1 - 100

(are there useful signatures?)

(are these classical or QM?)

Page 13: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

GHzCBA 25 Jmax 18

GHzCBA 10 Jmax 30

GHzCBA 3 Jmax 55

GHzCBA 1 Jmax 96

GHzCBA 1.0 Jmax 305

inertia of moment

1~constant Rotational

Spectra as a Function of Molecular Size

Population of levels

Page 14: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Atmospheric Propagation

Page 15: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Collisional Cooling: An Approach to Gas Phase Studies at Low Temperature

Atom Envy - Molecule Envy

Page 16: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Quantum Collisions

300 K 1 K_____________________

L ~ 30J ~ 10

L ~ 2J 1

Correspondence Principle

The predictions of the quantum theory for the behavior of any physical system must correspond to the prediction of classical physics in the limit in which the quantum numbers specifying the state of the system become very large.

hr ~ kT ~ Vwell

Page 17: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Typical Spectra - HCN

Page 18: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Sources and Metrology for the THzSynthesized Frequency Multiplication

Page 19: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Jumping the THz via Frequency SynthesisSpectroscopy via Photomixing

Fre

qu

ency

Ref

eren

ce

Sp

ectr

osc

op

ic M

easu

rem

ent

“Speed of Light from Direct Frequency and Wavelength Measurements of the Methane-Stabilized Laser,”

K. M. Evenson, J. S. Wells, F. R. Petersen, B. L. Danielson, G. W. Lay, R. L. Barger, and J. L. Hall,

Phys. Rev. Lett. 29, 1346-1349 (1972).

Page 20: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

VCO FrequencyReference10.5 GHz

Mixer

X8 MultiplierW-band

W-band Amplifier75-110 GHz

X3 MultiplierW-band

AmplifierLow Pass Filter10kHz – 1MHz

Harmonic10 MHz Comb

GeneratorAmplifierMixer

Gas Cell Detector

Computer DAQ

FrequencyStandard

x24

The Multiplied FASSST Spectrometer

105 resolution elements/sec

Page 21: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

The Fundamental FASSST Spectrometer

Page 22: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

“Frequency and phase-lock control of a 3 THz quantum cascade laser.”

A. L. Betz, R. T. Boreiko, B. S. Williams, S. Kumar, Q. Hu, J. L. Reno.

Opt Lett. 30, 1837-9 (2005).

Frequency Control and Reference in the THz

“A Tunable Cavity-Locked Diode Laser Source for Terahertz Photomixing,”

S. Matsuura, P. Chen, G. A. Blake, J. C. Pearson, and H. M. Pickett,

IEEE Trans. Microwave Theory and Tech. 48, 380 (2000).

Page 23: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Frequency Synthesis via Femtosecond Demodulation

“Microwave generation from picosecond demodulation sources”

F. C. De Lucia, B. D. Guenther, and T. Anderson

Appl. Phys. Lett. 47, 894 (1985)

I(f)

f “Spectral Purity and Sources of Noise in Femtosecond-Demodulation Terahertz Sources Drive by Ti:Sapphire Mode-Locked Lasers”

J. R. Demers, T. M. Goyette, Kyle B. Ferrio, H. O. Everitt, B. D. Guenther, and F. C. De Lucia

IEEE J. Quant. Electron. 37, (2004).

Page 24: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

“Optical frequency synthesis based on mode-locked lasers”

S. T. Cundiff, J. Ye, and J. L. Hall

Rev. Sci. Instrum. 72, 3749 (2001)

THz Synthesis from the Optical Comb

As with Evenson, THz mixer bandwidth and efficiency highly desirable

Page 25: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics
Page 26: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Atmospheric Remote Sensing

JPL - Microwave Limb Sounder

Ozone Destruction

Cycle

Page 27: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Microwave Limb Sounder

Page 28: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Image courtesy of NRAO/AUI and Computer graphics by ESO

Page 29: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

“Generation and Distribution of the mm-wave Reference Signal for ALMA”M. Musha, Y. Sato, K. Nakagawa, K. Ueda, A. Ueda, and M. IshiguroNMIJ-BIPM Workshop, Tsukuba 2004

Page 30: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Orion. IRAM 30-m telescope line survey

Page 31: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

“Whispered Excitement about the THz”

Graham Jordan Opening Plenary Presentation SPIE Symposium: Optics/Photonics in Security and Defense Bruges, Belgium, 26 September, 2005

‘New’ Applications - Holy Grails

How do we Move Beyond

to

A Field with many ‘Public’ Applications?

Page 32: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

The New York Times - July 11, 2005High-Tech Antiterror Tools: A Costly,

Long-Range Goal

Millimeter wave machines . . .use trace amounts of heat released by objects . . .to create images that can identify hidden bombs . . . from about 30 feet away.

Terahertz radiation devices can create images of concealed objects as well as identify the elemental components of a hidden item.

The terahertz devices may be more promising since they could sound an alarm if someone entering a subway or train station had traces of elements used in bombs on them.

Resolution

Spectroscopic Identification

Penetration

Page 33: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method To be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical) XMutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificity XClassical imaging XPoint gas detection

absolute specificity XAstrophysics (>$2x109) XAtmospheric (>$n x 108) XRemote gas detection

modest specificity X specificity in mixtures at 1km X

See through walls ~100 GHz >1 THz

Buried land mines> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill XExplosives/other solids close, sm obstruct, mixtures XExplosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

Page 34: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Cost? Size? Speed?

Breadth of Application?

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method To be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical) XMutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificity XClassical imaging XPoint gas detection

absolute specificity XAstrophysics (>$2x109) XAtmospheric (>$n x 108) XRemote gas detection

modest specificity XSee through walls ~100 GHz >1

THzBuried land mines

> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill XExplosives/other solids close, sm obstruct, mixtures XExplosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

Legacy Applications

Page 35: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method To be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical)Mutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificityClassical imaging XRemote gas detection X

modest specificityAstrophysics (>$2x109) XAtmospheric (>$n x 108) XSee through walls ~100 GHz >1

THzPoint gas detection

absolute specificity XBuried land mines

> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill XExplosives/other solids close, sm obstruct, mixtures XExplosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

Page 36: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method to be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical) XMutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificity XClassical imaging XRemote gas detection

modest specificity XPoint gas detection

absolute specificity XAstrophysics (>$2x109) XAtmospheric (>$n x 108) XSee through walls ~100 GHz >1

THzBuried land mines

> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill XExplosives/other solids close, sm obstruct, mixtures XExplosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

“it could be used to scan for diseases, such as cancer, the cells of which have a vibrant terahertz signature.”“New-wave body imaging -

medical imaging using Terahertz radiation”

e20 attenuation in 1 mm

Page 37: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method To be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical)Mutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificity XAstrophysics (>$2x109) XAtmospheric (>$n x 108) XClassical imaging T&SRemote gas detection

modest specificity T&SSee through walls ~100 GHz >1

THzPoint gas detection

absolute specificity XBuried land mines

> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill X

Explosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

“A camera that can see through clothes, skin and even walls without X-rays has been developed in what is being called one of the first great technological breakthroughs of the 21st century”

Page 38: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Impact Order demonstrated demonstrated clear path PhenomenaVLP

($spent or $potential) best method To be demo

Cancer/deep(spectra) XCancer/surface(spectra) XT-Ray (deep medical)Mutation(spectra) XBroadband communications ~100 GHz >1 THzExplosives remote with specificity XAstrophysics (>$2x109) XAtmospheric (>$n x 108) XClassical imaging T&SRemote gas detection

modest specificity T&SSee through walls ~100 GHz >1

THzPoint gas detection

absolute specificity XBuried land mines

> 6” ~100 GHz > 1THz< 6” >1 THz

Cancer/surface (water) XIncapacitate and kill XExplosives/other solids close, sm obstruct, mixtures XExplosives close, sort, sm obstruct some materialsPharmaceuticals, bio close, sort, sm obstruct some materials

“Since cancerous tissue tends to have a higher water content than healthy tissue, terahertz radiation could be used to differentiate between the two.”

?

A Good Challenge

Page 39: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

Signatures: Explosives Spectra

Clearly spurious results in both gas and

solids have been reported

Page 40: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

How do you look at THz images?

Page 41: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics
Page 42: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics
Page 43: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

What is so favorable about the SMM/THz?What are the Opportunities?

The SMM/THz combines penetrability with -a reasonable diffraction limit -a spectroscopic capability -low pressure gases have strong, redundant, unique signatures

-solids can have low lying vibrational modes, especially at high THz frequencies

Rotational transition strengths peak in the SMM/THz

The SMM/THz is very quiet: 1 mW/MHz => 1014 K

The commercial wireless market will provide us with a cheap technology

It should be possible to engineer small (because of the short wavelength), high spectral purity (because we can derive via multiplication from rf reference) and low power (because the background is quiet/the quanta is small) devices and systems

Page 44: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics

What is so Challenging about the SMM/THz?

Efficient generation of significant tunable, spectrally pure power levels

Practical broadband frequency control and measurement

The need to develop systems without knowledge of the phenomenology

Impact of the atmosphere

Page 45: Terahertz Spectroscopy and Applications Frank C. De Lucia Department of Physics