Optical pulse pair generator, light detection device, and light detection method

Patent metadata

Field	Value
Publication number	US-11909164-B2
Application number	US-201917054849-A
Country	US
Kind code	B2
Filing date	Apr 19, 2019
Priority date	May 14, 2018
Publication date	Feb 20, 2024
Grant date	Feb 20, 2024

Abstract

An optical pulse pair generator is configured to generate an optical pulse pair including a first pulse beam and a second pulse beam having respective central wavelengths that are separated by a predetermined wavelength difference from each other and having target time waveforms that are substantially the same as each other. The optical pulse pair generator provided includes a splitter section configured to split an incident pulse beam into two, a first shaping section configured to shape one of the pulse beams split by the splitter section by shaping into the target time waveform and setting a central frequency so as to configure the first pulse beam, and a second shaping section configured to shape the other of the pulse beams split by the splitter section by shaping into the target time waveform so as to configure the second pulse beam.

First claim

The invention claimed is:

1. An optical pulse pair generator configured to generate an optical pulse pair including a first pulse beam and a second pulse beam having respective central wavelengths that are separated by a predetermined wavelength difference from each other and having target time waveforms that are substantially the same as each other, the optical pulse pair generator comprising:
a splitter section configured to split an incident pulse beam into two;
a first shaping section configured to shape one of the pulse beams split by the splitter section by shaping into the target time waveform and setting a central frequency so as to configure the first pulse beam; and
a second shaping section configured to shape the other of the pulse beams split by the splitter section by shaping into the target time waveform so as to configure the second pulse beam,
wherein the first pulse beam and the second pulse beam both have an asymmetric waveform with a fall time that is longer than a rise time, and are temporally superimposed on each other.

2. The optical pulse pair generator of claim 1 , wherein:
the first shaping section includes a first bandpass filter having a bandwidth corresponding to the target time waveform of the one pulse beam and rotatable in a direction intersecting a propagation direction of the one pulse beam, and further includes a delay member configured to impart a variable time delay to the one pulse beam; and
the second shaping section includes a second bandpass filter having a bandwidth corresponding to the target time waveform of the other pulse beam.

3. The optical pulse pair generator of claim 2 , wherein:
a wavelength scanning section for scanning the wavelength difference is configured by the first bandpass filter and the delay member;
the first pulse beam and the second pulse beam are temporally superimposed on each other; and
the wavelength scanning section sets the wavelength difference by using a rotation angle of the first bandpass filter, and compensates a time difference between the first pulse beam and the second pulse beam accompanying rotation of the first bandpass filter by using the time delay of the delay member.

4. The optical pulse pair generator of claim 2 , wherein the splitter section is configured by the second bandpass filter.

5. A light detection device comprising the optical pulse pair generator of claim 1 and configured to perform light detection using an excitation pulse beam, a first probe pulse beam, and a second probe pulse beam, wherein the first pulse beam configures the first probe pulse beam, the light detection device further comprising:
a laser light source configured to generate a light source pulse beam;
a light source splitter section configured to split the light source pulse beam in two by splitting into the excitation pulse beam and the incident pulse beam;
a modulation section configured to phase modulate the second pulse beam so as to configure the second probe pulse beam;
a multiplexing section configured to multiplex the excitation pulse beam, the first probe pulse beam, and the second probe pulse beam so as to generate a multiplexed beam;
an illumination section configured to illuminate a sample with the multiplexed beam; and
a detection section configured to employ heterodyne interference due to the first probe pulse beam and the second probe pulse beam to detect a molecular vibration excited by the excitation pulse beam when the multiplexed beam is illuminating the sample.

6. The light detection device of claim 5 , wherein the first probe pulse beam and the second probe pulse beam both have an asymmetric waveform with a fall time that is longer than a rise time, are temporally superimposed on each other, and are delayed by a predetermined delay time relative to the excitation pulse beam.

7. The light detection device of claim 5 , wherein:
the excitation pulse beam is polarized in advance;
a wavelength of the first probe pulse beam and a wavelength of the second probe pulse beam are different from each other;
the illumination section includes a microscope; and
the detection section includes a polarizer configured to remove the excitation pulse beam from the multiplexed beam after the sample has been illuminated, an optical filter configured to remove the second probe pulse beam from the multiplexed beam after the sample has been illuminated, and a light reception section configured to receive the first probe pulse beam.

8. The light detection device of claim 7 , wherein:
the first shaping section includes a wavelength scanning section configured to scan the wavelength difference, the wavelength scanning section including a first bandpass filter having a bandwidth corresponding to the target time waveform of the one pulse beam and rotatable in a direction intersecting a propagation direction of the first pulse beam, and further including a delay member configured to impart a variable time delay to the one pulse beam; and
the light detection device further comprises a control section configured to control the wavelength scanning section so as to set the wavelength difference by using a rotation angle of the first bandpass filter and to compensate a time difference between the first probe pulse beam and the second probe pulse beam accompanying rotation of the first bandpass filter by using the time delay of the delay member, and further configured to control the modulation section so as to perform phase modulation with a modulation signal having a saw-tooth waveform including regions of linear change in phase for the second probe pulse beam transmitted through a second bandpass filter having a bandwidth corresponding to the target time waveform and including connection regions at which there is a steep change of phase difference 2π.

9. The light detection device of claim 8 , wherein the control section is configured to accept a received light signal output from the light reception section, to configure a lock-in amplifier using the received light signal and the modulation signal, and to detect an amplitude-modulated signal from modulating the first probe pulse beam resulting from heterodyne interference due to the lock-in amplifier as a signal corresponding to a stimulated Raman scattering signal.

10. The light detection device of claim 9 , wherein:
the first bandpass filter applies a predetermined odd-number high order dispersion to the first probe pulse beam; and
the second bandpass filter applies the predetermined odd-number high order dispersion to the second probe pulse beam.

11. A method of detecting light of a molecular vibration using a light detection device including a laser light source configured to generate a light source pulse beam, a splitter section configured to split the light source pulse beam into three by splitting into an excitation pulse beam, and a first probe pulse beam and a second probe pulse beam that both have a predetermined waveform, a first shaping section configured to shape the first probe pulse beam by shaping into the predetermined waveform and setting a central frequency, a second shaping section configured to shape the second probe pulse beam by shaping into the predetermined waveform, a modulation section configured to phase modulate the second probe pulse beam, a multiplexing section configured to multiplex the excitation pulse beam, the first probe pulse beam, and the second probe pulse beam so as to generate a multiplexed beam, and an illumination section configured to illuminate a sample with the multiplexed beam, the light detection method comprising:
setting a difference between a central wavelength of the first probe pulse beam and a central wavelength of the secon

Assignees

• National Univ Corporation Tokyo Univ Of Agriculture & Technology
• National Univ Corporation Tokyo Univ Of Agriculture And Technology

Inventors

• Misawa Kazuhiko
• Ito Terumasa

Classifications

• H01S3/0057 Primary

  Temporal shaping, e.g. pulse compression, frequency chirping (soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108) · CPC title

• G01N21/65

  Raman scattering · CPC title

• G02B21/06

  Means for illuminating specimens · CPC title

• G02B27/1006

  for splitting or combining different wavelengths (G02B27/1086, G02B27/141 take precedence) · CPC title

• H01S3/0078

  Frequency filtering · CPC title