# US 12,007,274 B2 · Device and method for ultrashort pulse temporal measurement

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- Number: US 12,007,274 B2
- Document ID: US12007274B2
- Status: Granted
- Kind: B2
- Application number: 17/292,659
- Filed: 2018-11-08
- Published: 2022-01-13
- Granted: 2024-06-11
- Earliest claimed: 2018-11-08
- Assignees: Sphere Ultrafast Photonics, SA
- Applicants: Sphere Ultrafast Photonics SA
- Inventors: Miguel Nicolau Da Costa Ribeiro De Miranda; Chen Guo; Maïté Louisy; Cord Louis Arnold; Anne Genevieve L'Huillier Wahlstrom
- Web page: https://patentgrep.com/patent/US12007274B2

## CPC

- G01J 11/00: Measuring the characteristics of individual optical pulses or of optical pulse trains
- G01R 29/08: Measuring electromagnetic field characteristics
- G01J: MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY (light sources F21, H01J, H01K, H05B; investigating properties of materials by optical means G01N)
- G01R: MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES (indicating correct tuning of resonant circuits H03J3/12)

## Abstract

The present disclosure relates to laser systems and laser pulse measurement methods. The method comprises a dispersive system for applying a controlled chirp, to an incoming ultrashort light pulse to be measured; an optical system for selecting an homogeneous part of the transverse spatial beam profile of said light pulse; applying different spectral phases to different spatial parts of the beam obtained in the previous step, which comprises allowing different spatial parts of the beam to cross different thicknesses of material; focusing or propagating the beam in a nonlinear medium after applying the spectral phases; applying a nonlinear process to the pulse to be characterized for each spatial part of the beam, allowing the generation of a nonlinear signal for each spatial part of the beam; measuring the corresponding bi-dimensional data set that has the information on the nonlinear signal generated for each applied spectral phase in a detector; applying a numerical iterative algorithm to the measured data set to retrieve the spectral phase of the pulse to be characterized; such process being done in a parallel fashion.

## Claims

### Claim 1

A method for ultrashort pulse measurement comprising the following steps:
introducing a controlled chirp, negative or positive, to an incoming ultrashort light pulse to be measured;
selecting a homogeneous portion of the transverse spatial beam profile of said light pulse;
propagating the beam resulting from the previous step through an arrangement of optical elements for imparting different spectral phases to different spatial components of said beam;
applying a nonlinear optical process to the beam resulting from the previous step for each different spatial component of said beam;
recording a bi-dimensional set of data comprising the spectrum of the nonlinear signal generated for each different spatial component of said beam; and
calculating, by an electronic data processor, a numerical iterative algorithm to said recorded spectral image data, to retrieve the amplitude and phase of the electric field of the ultrashort light pulse.

### Claim 2 (depends on 1)

The method according to claim 1, further comprising, after imparting different spectral phases to different spatial components of said beam, projecting the different spatial components of said beam along a line before applying a nonlinear optical process for each different spatial component of said beam.

### Claim 3 (depends on 1)

The method according to claim 1, wherein the applied nonlinear process comprises second-harmonic generation or another nonlinear effect that affects the fundamental spectrum of the ultrashort light pulse selected from the group consisting of: sum-frequency generation, difference-frequency generation, the optical Kerr effect, self- and cross-phase modulation, cross-polarized wave generation, third- and higher-order harmonic generation, and combinations thereof.

### Claim 4 (depends on 1)

The method according to claim 1, comprising the use of means to execute in parallel said impartment of spectral phases, nonlinear optical process and recording of the resulting nonlinear signal generated for each different spatial component of said beam.

### Claim 5

A device for ultrashort pulse measurement, comprising:
an optical section for applying a controlled chirp, negative or positive, to an incoming ultrashort light pulse to be measured;
an optical section for selecting a homogeneous, central portion of the transverse spatial beam profile of said light pulse from the previous section;
an optical section to propagate the beam from the previous section through optical elements for imparting different spectral phases to different spatial components of said beam;
an optical section for applying a nonlinear process to the beam resulting from the previous section for each different spatial component of said beam;
a sensor for recording the bi-dimensional set of data comprising the spectrum of the nonlinear signal generated for different spatial component of said beam from the previous section; and
an electronic data processor configured for executing a numerical iterative algorithm, to said recorded spectral image recorded by said sensor, to retrieve the amplitude and phase of the electric field of the ultrashort light pulse.

### Claim 6 (depends on 5)

The device according to claim 5, wherein a section for projecting the different spatial components of said beam into a line is inserted after the optical section for imparting different spectral phases to different spatial components of said beam and before the section for applying a nonlinear optical process for each different spatial component of said beam.

### Claim 7 (depends on 6)

The device according to claim 6, wherein the optical section for projecting the different spatial components of said beam into a line comprises spherical minors, parabolic mirrors, spherical lenses, aspherical lenses, prisms, wedges, windows, plates, cylindrical lenses, or combinations thereof.

### Claim 8 (depends on 5)

The device according claim 5, wherein the optical section for applying a controlled chirp comprises a pulse compressor or a pulse stretcher.

### Claim 9 (depends on 8)

The device according to claim 8, wherein said pulse compressor or stretcher comprises chirped minors and glass wedges.

### Claim 10 (depends on 5)

The device according to claim 5, wherein the optical section for selecting a homogeneous portion of the transverse spatial beam profile of said light pulse comprises focusing mirrors, lenses, prisms, wedges, windows, plates, or combinations thereof.

### Claim 11 (depends on 5)

The device according to claim 5, wherein the optical section that allows imparting different spectral phases to different spatial components of the beam comprises materials in different thicknesses, wedges, prisms, grisms, diffraction gratings, and/or optical modulators such as acousto-optic, electro-optic and/or liquid crystal based devices, or combinations thereof.

### Claim 12 (depends on 5)

The device according to claim 5, wherein the applied nonlinear process comprises second-harmonic generation or any other nonlinear effect that affects the fundamental spectrum of the ultrashort light pulse, comprising sum-frequency generation, difference-frequency generation, the optical Kerr effect, self- and cross-phase modulation, cross-polarized wave generation, third- and higher-order harmonic generation, or combinations thereof, taking place in gases, solids, liquids or plasmas.

### Claim 13 (depends on 5)

The device according to claim 5, wherein the numerical iterative algorithm comprises a Multiphoton Intrapulse Interference Phase Scan, MIIPS algorithm, a Chirp Reversal Technique, CRT algorithm, a dispersion-scan, a d-scan algorithm, or a combination thereof.

### Claim 14 (depends on 5)

The device according to claim 5, comprising means to execute in parallel said impartment of spectral phases, nonlinear conversion and measurement of the resulting signal.

### Claim 15 (depends on 5)

The device according to claim 5, wherein the incoming ultrashort light pulse to be measured does not have to pass through maximum compression to perform the measurement.