Method and device for cavity-enhanced broadband intrapulse difference frequency generation

Patent metadata

Field	Value
Publication number	US-10042231-B2
Application number	US-201515503432-A
Country	US
Kind code	B2
Filing date	Jul 13, 2015
Priority date	Aug 25, 2014
Publication date	Aug 7, 2018
Grant date	Aug 7, 2018

Abstract

A method of creating difference frequency (DF) laser pulses ( 1 ) by difference frequency generation (DFG) comprises the steps of providing ultrashort laser pulses ( 2 ) having a spectral bandwidth corresponding to a Fourier limit of below 50 fs and containing first spectral components and second spectral components having larger frequencies than the first spectral components, and driving a DFG process by the ultrashort laser pulses ( 2 ) in an optically non-linear crystal ( 10 ), wherein the DF laser pulses ( 1 ) are generated in the crystal ( 10 ) by difference frequencies between the first and second spectral components, resp., said difference frequencies comprising third spectral components being lower in frequency than the first and second spectral components, wherein at least one enhancement cavity ( 20 ) with resonator mirrors (Mi 1 to M 14 ) spanning a beam path ( 22 ) is provided and the crystal ( 10 ) is placed in the beam path ( 22 ) of the enhancement cavity ( 20 ), the ultrashort laser pulses ( 2 ) are input coupled and coherently added in the at least one enhancement cavity ( 20 ), at least one circulating ultrashort laser pulse ( 3 ) is created in the at least one enhancement cavity ( 20 ), which drives the DFG process in the crystal ( 10 ) for generating the DF laser pulses ( 1 ), and the at least one enhancement cavity ( 20 ) is adapted for recycling the at least one ultrashort laser pulse ( 3 ) passing through the crystal ( 10 ). Furthermore, a photonic source ( 100 ) for creating DF laser pulses ( 1 ) is described, including one or more enhancement cavities.

First claim

The invention claimed is:

1. A method of creating difference frequency (DF) laser pulses by difference frequency generation (DFG), comprising the steps of
providing a first femtosecond enhancement cavity with first resonator mirrors spanning a first beam path,
providing ultrashort laser pulses having a spectral bandwidth corresponding to a Fourier limit of below 20 fs and simultaneously containing first spectral components and second spectral components having larger frequencies than the first spectral components, wherein the first femtosecond enhancement cavity is configured for a coherent superposition of the ultrashort laser pulses,
input coupling and coherently adding of the ultrashort laser pulses in the first femtosecond enhancement cavity,
driving a DFG process by the ultrashort laser pulses in a first optically non-linear crystal being placed in the first beam path of the first femtosecond enhancement cavity, wherein the DF laser pulses are created in the first optically non-linear crystal by difference frequencies between the first and second spectral components, respectively, said difference frequencies comprising third spectral components being lower in frequency than both of the first and second spectral components,
wherein at least one circulating ultrashort laser pulse is created in the first femtosecond enhancement cavity, which drives the DFG process in the first optically non-linear crystal for generating the DF laser pulses, and the first femtosecond enhancement cavity is configured for recycling the at least one ultrashort laser pulse passing through the first optically non-linear crystal, and
output coupling of the DF laser pulses from the first femtosecond enhancement cavity, wherein the DF laser pulses have a center wavelength in a range of 4 μm to 20 μm and a spectral width of at least 500 nm.

2. The method according to claim 1 , wherein the step of output coupling of the DF laser pulses comprises
reflecting the DF laser pulses out of the first beam path at a reflecting dichroic surface on a rear side of the first optically non-linear crystal and an antireflective coating on a front side of the first optically non-linear crystal.

3. The method according to claim 1 , wherein the step of output coupling of the DF laser pulses comprises
transmitting the DF laser pulses out of the first beam path through a dichroic surface of the first resonator mirror downstream of the first optically non-linear crystal.

4. The method according to claim 1 , wherein the step of output coupling of the DF laser pulses comprises
reflecting the DF laser pulses out of the first beam path at a surface of a dichroic plate arranged in the first femtosecond enhancement cavity.

5. The method according to claim 1 , wherein the step of output coupling of the DF laser pulses comprises
relaying a divergent portion of the DF laser pulses over one of the first resonator mirrors or an auxiliary mirror with a hole transmitting the circulating ultrashort laser pulse in the first femtosecond enhancement cavity.

6. The method according to claim 1 , wherein the step of providing the ultrashort laser pulses comprises
generating the ultrashort laser pulses with one single laser source.

7. The method according to claim 1 , wherein the step of providing the ultrashort laser pulses comprises
suppressing spectral components of the ultrashort laser pulses, which do not contribute to the DFG process.

8. The method according to claim 1 , including a step of
adjusting a polarization of the first spectral components relative to a polarization of the second spectral components of the ultrashort laser pulses, so that the polarizations of the first and second spectral components are parallel or perpendicular relative to each other.

9. The method according to claim 8 , wherein the polarizations of the first and second spectral components are adjusted before input coupling the ultrashort laser pulses into the first femtosecond enhancement cavity.

10. The method according to claim 1 , including a step of
placing a second optically non-linear crystal in the first beam path of the first femtosecond enhancement cavity, the second optically non-linear crystal being configured for compensating for an ellipticity of a polarization of the light field circulating in the first femtosecond enhancement cavity, said ellipticity being generated in the first optically non-linear crystal.

11. The method according to claim 10 , wherein
the second optically non-linear crystal is further configured for creating further difference frequencies within the third spectral component by difference frequency generation.

12. The method according to claim 1 , including further steps of
providing one or more further femtosecond enhancement cavities spanning one or more further beam paths, wherein each of the one or more further femtosecond enhancement cavities is arranged relative to the first femtosecond enhancement cavity such that the first optically non-linear crystal is placed at an intersection of all of the first and the one or more further beam paths of the first and the one or more further femtosecond enhancement cavities,
providing two or more pulse portions by wavelength selective splitting of the ultrashort laser pulses, wherein spectral content of the first and second spectral components is distributed into the two or more pulse portions,
input coupling each of the two or more pulse portions into one of the first and the one or more further femtosecond enhancement cavities and coherently adding the two or more pulse portions to at least two circulating ultrashort laser pulses each of which circulating in one of the first and the one or more further femtosecond enhancement cavities, respectively, wherein
the polarizations of the two or more pulse portions are adjusted such that the two or more circulating ultrashort laser pulses in the first and the one or more further femtosecond enhancement cavities have different polarizations at the first optically non-linear crystal, and
the DFG process is driven in the first optically non-linear crystal by the two or more circulating ultrashort laser pulses.

13. The method according to claim 12 , wherein
the one or more further femtosecond enhancement cavities is at least two further femtosecond enhancement cavities, and each of the at least two further femtosecond enhancement cavities is arranged for coherently adding pulse portions with different spectral content and different polarizations.

14. The method according to claim 1 , wherein
the first optically nonlinear crystal has a thickness in a range of 5 μm to 5 mm.

15. The method according to claim 1 , wherein
the first optically nonlinear crystal is in direct contact with one of the resonator mirrors.

16. The method according to claim 1 , wherein
a temperature of the first optically non-linear crystal is set by one of the first resonator mirrors or a temperature-control support stage, wherein the first optically non-linear crystal is optically contacted or attached to the one of the first resonator mirrors or the temperature-control support stage.

17. The method according to claim 1 , wherein
an adjusting support stage of the first optically non-linear crystal is controlled for adjusting an orientation of the first optically non-linear crystal with respect to the first beam path of the first femtosecond enhancement cavity.

18. The method according to claim 1 , wherein
the first femtosecond enhancement cavity is operated in an evacuated environment.

19. A p

Assignees

• Max Planck Gesellschaft
• Univ Muenchen Ludwig Maximilians
• Max Planck Gesellschaft

Inventors

• Apolonskiy Alexander
• Fill Ernst
• Pupeza Ioachim
• Krausz Ferenc

Classifications

• G02F1/3534 Primary

  Three-wave interaction, e.g. sum-difference frequency generation (G02F1/3532 takes precedence) · CPC title

• G02F1/3501

  Constructional details or arrangements of non-linear optical devices, e.g. shape of non-linear crystals · CPC title

• G02F2203/15

  involving resonance effects, e.g. resonantly enhanced interaction · CPC title

• G02F2001/3503

  Physics · mapped topic

• G02F2001/3542

  Physics · mapped topic