Airy beam light sheet and airy beam light sheet microscope

Patent metadata

Field	Value
Publication number	US-10816787-B2
Application number	US-201916433429-A
Country	US
Kind code	B2
Filing date	Jun 6, 2019
Priority date	Jul 30, 2014
Publication date	Oct 27, 2020
Grant date	Oct 27, 2020

Abstract

An optical system for generating an Airy beam light sheet comprising an optical arrangement for generating a Gaussian beam, and an optical element for converting the Gaussian beam into an Airy beam light sheet, wherein a single optical element is provided for converting the Gaussian beam into an Airy beam light sheet.

First claim

The invention claimed is:

1. A method for generating a modulated Airy beam or a modulated Airy beam light sheet, the method comprising:
generating a Gaussian beam; and
imparting, on the Gaussian beam, a cubic phase modulation and a further modulation in phase and/or amplitude, which further modulation is additional to the cubic phase modulation, to thereby convert the Gaussian beam into a modulated Airy beam or a modulated Airy beam light sheet,
wherein the further modulation in phase and/or amplitude is selected so as to provide the modulated Airy beam or the modulated Airy beam light sheet with an intensity profile that increases in a direction of propagation of the modulated Airy beam or the modulated Airy beam light sheet, or
wherein the further modulation in phase and/or amplitude is selected so as to at least partially compensate for attenuation or scattering losses experienced by the modulated Airy beam or the modulated Airy beam light sheet during propagation of the modulated Airy beam or the modulated Airy beam light sheet in a lossy medium.

2. A method as claimed in claim 1 , comprising:
multiplying an Airy beam spatial spectral function by a spatial spectral modulation function, thereby to produce the modulated Airy beam or the modulated Airy beam light sheet, wherein the Airy beam spatial spectral function is associated with the cubic phase modulation, and the spatial spectral modulation function is associated with the further modulation in phase and/or amplitude.

3. A method as claimed in claim 1 , comprising using a modulation arrangement to impart, on the Gaussian beam, the cubic phase modulation and the further modulation in phase and/or amplitude.

4. A method as claimed in claim 3 , wherein the modulation arrangement comprises at least one of a diffractive optical element, a spatial light modulator and a digital micromirror device.

5. A method as claimed in claim 1 , comprising using an optical element to impart the cubic phase modulation on the Gaussian beam thereby to convert the Gaussian beam to an Airy beam or an Airy beam light sheet, wherein the optical element is a unitary optical element.

6. A method as claimed in claim 5 , wherein the optical element comprises a static optical element and/or a passive diffractive optical element.

7. A method as claimed in claim 5 , wherein the optical element comprises a cylindrical lens that is tilted relative to a direction of propagation of the Gaussian beam.

8. A method as claimed in claim 5 , comprising using a modulation device or a modulation element to impart the further modulation in phase and/or amplitude of the Airy beam light sheet to provide a desired intensity modulation.

9. A method as claimed in claim 8 , wherein the modulation device or the modulation element comprises at least one of a diffractive optical element, a spatial light modulator, a digital micromirror device and a variable attenuator.

10. A method as claimed in claim 8 , wherein the modulation device or the modulation element is positioned before the optical element.

11. A method as claimed in claim 1 , wherein the further modulation in phase and/or amplitude is selected so as to provide the modulated Airy beam or the modulated Airy beam light sheet with a peak intensity that increases in the direction of propagation of the modulated Airy beam or the modulated Airy beam light sheet.

12. A method as claimed in claim 1 , wherein the further modulation in phase and/or amplitude is selected so as to at least partially compensate for attenuation or scattering losses experienced by a peak intensity of the modulated Airy beam or the modulated Airy beam light sheet during propagation of the modulated Airy beam or the modulated Airy beam light sheet in the lossy medium.

13. A method as claimed in claim 2 , wherein the spectral modulation function is associated with a modulation in amplitude which is represented by exp(−b 0 k x ), where k x represents a wave-vector associated with a direction x which is transverse to a propagation direction z of the modulated Airy beam or the modulated Airy beam light sheet and where b 0 is a constant.

14. A method for generating a modulated Airy beam or a modulated Airy beam light sheet, the method comprising:
generating a Gaussian beam; and
imparting, on the Gaussian beam, a spatial modulation to thereby convert the Gaussian beam into a modulated Airy beam or a modulated Airy beam light sheet,
wherein the modulated Airy beam or the modulated Airy beam light sheet is defined by a spectral function which is a function of an Airy beam spectral function multiplied by a spectral modulation function,
wherein the Airy beam spectral function is associated with a cubic phase modulation, and
wherein the spectral modulation function is associated with a further modulation in phase and/or amplitude which is additional to the cubic phase modulation.

15. A method as claimed in claim 14 , wherein the spectral modulation function is associated with a modulation in amplitude which is represented by exp(−b 0 k x ), where k x represents a wave-vector associated with a direction x which is transverse to a propagation direction z of the modulated Airy beam or the modulated Airy beam light sheet and where b 0 is a constant.

16. A method as claimed in claim 14 , wherein the further modulation in phase and/or amplitude is selected so as to provide the modulated Airy beam or the modulated Airy beam light sheet with an intensity profile that increases in a direction of propagation of the modulated Airy beam or the modulated Airy beam light sheet.

17. A method as claimed in claim 16 , wherein the further modulation in phase and/or amplitude is selected so as to provide the modulated Airy beam or the modulated Airy beam light sheet with a peak intensity that increases in the direction of propagation of the modulated Airy beam or the modulated Airy beam light sheet.

18. A method as claimed in claim 14 , wherein the further modulation in phase and/or amplitude is selected so as to at least partially compensate for attenuation or scattering losses experienced by the modulated Airy beam or the modulated Airy beam light sheet during propagation of the modulated Airy beam or the modulated Airy beam light sheet in a lossy medium.

19. A method as claimed in claim 18 , wherein the further modulation in phase and/or amplitude is selected so as to at least partially compensate for attenuation or scattering losses experienced by a peak intensity of the modulated Airy beam or the modulated Airy beam light sheet during propagation of the modulated Airy beam or the modulated Airy beam light sheet in the lossy medium.

Assignees

• Univ Court Univ St Andrews
• Univ Court Of The Univ Of St Andrew

Inventors

• Mazilu Michael
• Vettenburg Tom
• Dholakia Kishan
• Preciado Miguel
• Yang Zhengyi

Classifications

• G02B21/0032 Primary

  Optical details of illumination, e.g. light-sources, pinholes, beam splitters, slits, fibers (G02B21/0036 - G02B21/008; means for illumination of specimens in general G02B21/06) · CPC title

• G02B27/0927

  Systems for changing the beam intensity distribution, e.g. Gaussian to top-hat · CPC title

• G02B27/0966

  Cylindrical lenses (cylindrical lenses per se G02B3/06) · CPC title

• G02B26/06

  for controlling the phase of light (G02B26/08 takes precedence {, measuring optical phase difference G01J9/00}) · CPC title

• G02B26/02

  for controlling the intensity of light {(G02B26/004 takes precedence)} · CPC title