Optoacoustic spectroscopy of condensed matter in bulk form

• US 4,303,343 A
• Filed: 02/29/1980
• Issued: 12/01/1981
• Est. Priority Date: 02/29/1980
• Status: Expired due to Term

• Current Assignee: Bell Telephone Laboratories, Inc. (Nokia Corporation)
• Original Assignee: Bell Telephone Laboratories, Inc. (Nokia Corporation)
• Inventors: Tam, Andrew C., Patel, Chandra K. N.
• Primary Examiner(s): ROSENBERGER, RICHARD A
• Application Number:
  US06/125,985
• Time in Patent Office: 641 Days
• Field of Search: 356/432, 250/351
• US Class Current: 356/432
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids
• CPC Class Codes: G01N 2291/0421 Longitudinal waves
• CPC Class Codes: G01N 29/00 Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object G01N3/00, G01N5/00, G01N7/00, G01N9/00, G01N11/00, G01N13/00, G01N15/00, G01N17/00, G01N19/00, G01N21/00, G01N22/00, G01N23/00, G01N24/00, G01N25/00, G01N27/00 take precedence
• CPC Class Codes: G01N 29/2418 using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046

Abstract

Method and apparatus for high-sensitivity (α≲10^-6 cm^-1) optoacoustic (OA) spectroscopy of substantially transparent bulk condensed matter. Part of the sample to be investigated is irradiated by pulses of radiation, typically from a pulsed dye laser. The small amount of energy absorbed by the sample causes thermal expansion of the irradiated region, resulting in cylindrical stress waves being radiated from that region. These stress waves can be observed with appropriate detection means at a location remote from the source. The method is applicable to essentially transparent liquids, and solids, and to absorptive solids suspended in liquids, and the like. Possible choices of probe radiation are not only the conventional ones of visible, near UV, and near infrared electromagnetic radiation, but also, for instance, γ-rays, x-rays, vacuum UV, and far infrared. Two conditions are shown to exist that relate pulse duration, beam size, and various material parameters, observation of which results in optimization of the sensitivity of the method, and the sensitivity is typically highest for pulses having duration of about 10^-7 sec-10^-4 sec.

Claims

1. An improved method for optoacoustic spectroscopy of a bulk sample of relatively transparent condensed matter comprising

(a) irradiating at least a part of the sample, the source region, with a pulsed beam of radiation of frequency ν

and pulse length τ

_p, with pulse rate ν

_R,

(b) limiting the beam dimensions to a maximum cross-sectional dimension of the source region L_m, and

(c) detecting elastic waves generated in the sample that have propagated to the detecting means substantially only through condensed matter,

wherein the improvement comprises

(d) adjusting τ

_p to be between about 10^-7 and 10^-4 seconds.

(e) adjusting ν

_R to be much less than about τ

_p^-1, and

(f) adjusting the beam such that L_m ≲

vτ

_p, and simultaneously L_m to be much greater than about (4τ

_p D)^1/2, where

v is the phase velocity in the sample of elastic compressional waves, and

D is the thermal diffusivity of the sample material.

2. Method according to claim 1, further comprising adjusting the energy in the pulse E_o that (α

(ν

)lE_o ν

_R /V)≲

10^-6 watt/cm³, where α

(ν

) is the absorption coefficient of the sample,

l is the length of the source region in the sample,

ν

_R is the pulse rate, and

V is the sample volume.

3. An improved apparatus for optoacoustic spectroscopy of a bulk sample of relatively transparent condensed bulk matter comprising

(a) means for irradiating at least a part of the sample, the sample source region, with a pulsed beam of radiation of frequency ν

and pulse length τ

_p, with pulse rate ν

_R,

(b) means for limiting the beam dimensions to a maximum cross-sectional dimension of the source region L_m, and

(c) means for detecting elastic waves generated in the sample that have propagated to the detecting means substantially only through condensed matter,

wherein the improvement comprises

(d) means for adjusting τ

_p to be between about 10^-7 and 10^-4 seconds,

(e) means for adjusting ν

_R to be much less than about τ

_p^-1, and

(f) means for adjusting the beam-dimension-limiting means such that I_m ≲

vτ

_p, and simultaneously L_m to be much greater than about (4τ

_p D)^1/2, where

v is the phase velocity in the sample of elastic compressional waves, and

D is the thermal diffusivity of the sample material.

4. Aparatus according to claim 3, further comprising means for adjusting the energy in the pulse E_o such that (α

(ν

)lE_o ν

_R /V)≲

10^-6 watt/cm^-3, where

α

(ν

) is the absorption coefficient of the sample,

l is the length of the source region in the sample,

ν

_R is the pulse rate, and

V is the sample volume.

5. Apparatus according to claim 3 wherein the irradiating means comprise a pulsed laser.

6. Apparatus according to claim 3 wherein the irradiating means comprise a pulsed arc lamp.

7. Apparatus according to claim 5 wherein the pulsed laser is a dye laser having a pulse length of the order of 10^-6 sec and a repetition rate of the order of 10 sec^-1.

8. Apparatus according to claim 3 wherein the radiation used is γ

-, X-, vacuum UV, UV, infrared, or far infrared radiation.