Rotationally tunable optical delay line

• US 7,643,212 B1
• Filed: 10/09/2008
• Issued: 01/05/2010
• Est. Priority Date: 10/10/2007
• Status: Expired due to Fees

• Current Assignee: Jason P. Sokoloff, Lawrence Sokoloff
• Original Assignee: Jason P. Sokoloff, Lawrence Sokoloff
• Inventors: Sokoloff, Jason P., Sokoloff, Lawrence
• Primary Examiner(s): Lee (Andrew); Hwa S
• Application Number:
  US12/287,416
• Time in Patent Office: 453 Days
• Field of Search: 372/20, 372/21, 372/27
• US Class Current: 359/490.02
• CPC Class Codes: G02B 26/0883 the refracting element being a prism

Abstract

A rotationally tunable time delay line device for providing a continually adjustable time delay between two orthogonally polarized laser pulses is described. The device is comprised of one or more rotational delay crystals, each made of a flat uniaxially birefringent crystal with a special orientation of its internal optical axis. The time delay generated between the two orthogonally polarized laser pulses that travel through the rotationally tunable delay line can be continually adjusted by rotating the constituent rotational delay crystals around their surface normals. An application is demonstrated in detail where the rotationally tunable time delay line device is used to form an optical autocorrelator for measuring femtosecond or picosecond duration laser pulses.

Claims

1. A tunable optical rotational delay line apparatus for providing a continually adjustable time delay between two orthogonally polarized co-linear laser pulses, the rotational delay line apparatus comprising:

a. a rotational delay crystal made of a parallel flat birefringent crystal having an ordinary refractiveindex n_o and extra-ordinary refractive index n_e, wherein

the unique optic axis of said rotational delay crystal is oriented at an angle β

to the rotational delay crystal surface normal, where β

is greater than 0 degrees and less than 90 degrees;

b. a means of rotating said rotational delay crystal about its surface normal;

c. whereby a time delay between said two orthogonally polarized co-linear laser pulses that travel through said rotational delay crystal can be continually adjusted by

i. inclining said surface normal of said rotational delay crystal at an angle θ

to the direction of travel of said co-linear laser pulses, where θ

=n_o sin(β

);

ii. rotating said rotational delay crystal about its surface normal.

2. The apparatus as defined in claim 1, further comprising a second rotational delay crystal identical to the first rotational delay crystal, wherein said second rotational delay crystal is rotated and fixed adjacent to said first rotational delay so that the angle formed by said first rotational delay crystal'"'"'s unique optic axis and said second rotational delay crystal'"'"'s unique optic axis is 2β

and is bisected by said common surface normal.

3. The apparatus as defined in claim 1, wherein said flat birefringent crystal is selected from the group consisting of calcite crystal, quartz crystal, alpha-barium borate (alpha-BBO) crystal, rutile, and yttrium orthovanadate (YVO4) crystal.

4. The apparatus as defined in claim 1, where β

is approximately between 10 and 60 degrees.

5. An autocorrelator for measuring a laser pulse comprising:

a. a circular polarizer;

b. a rotational delay crystal made of a parallel flat birefringent crystal having an ordinary refractive index n_o and extra-ordinary refractive index n_e, wherein

the unique optic axis of said rotational delay crystal is oriented at an angle β

to the rotational delay crystal surface normal, where β

is between 0 and 90 degrees;

c. a means of rotating said rotational delay crystal;

d. a focusing lens; and

a

e. photodetector unit

f. wherein said circular polarizer changes an incident light ray into two orthogonally polarized collinear rays;

g. whereby a time delay between said two orthogonally polarized co-linear laser pulses that travel through said rotational delay crystal can be continually adjusted by

i. inclining said surface normal of said rotational delay crystal at an angle θ

to the direction of travel of said co-linear laser pulses, where θ

=n_o sin(β

);

ii. rotating said rotational delay crystal about its surface normal;

iii. whereby said focusing lens focuses said two orthogonally polarized laser pulses onto said photodetector unit and said photodetector unit generates an electrical current proportional to said time delay generated by said rotational delay crystal.

6. The autocorrelator as defined in claim 5, wherein a second rotational delay crystal identical to the first rotational delay crystal is rotated and fixed adjacent to said first rotational delay so that the angle formed by said first rotational delay crystal'"'"'s unique optic axis and said second rotational delay crystal'"'"'s unique optic axis is 2β

and is bisected by said common surface normal.

7. The autocorrelator as defined in claim 6, wherein said flat birefringent crystal is selected from the group consisting of calcite crystal, quartz crystal, alpha-barium borate (alpha-BBO) crystal, rutile, and yttrium orthovanadate (YVO4) crystal.

8. The autocorrelator as claimed in claim 6 further comprising a quarter wave plate and polarizer sequentially arranged and interposed between said second rotational delay crystal and said focusing lens.

9. The autocorrelator as claimed in claim 6 wherein said circular polarizer is a comprised of a polarization beamsplitter and quarter wave plate;

and further comprising a retroreflector located behind said first and second rotational delay crystals whereby said retroreflector reflects light on a return path to said polarizing beam splitter whereby one polarization of said reflected light is directed by said polarization beam splitter to said focusing lens and said photodetector unit.

10. The autocorrelator as claimed in claim 9 wherein said retroreflector is a mirror.

11. A method of generating a time delay between two orthogonally polarized light pulses comprising

a. inclining the surface normal of a flat birefringent crystal at an angle θ

to the direction of travel of the incident light pulses said birefringent crystal having an internal unique optic axis oriented relative to said surface normal of said birefringent crystal at an angle of β

=arcsin(θ

)/n_o where θ

is such that β

is greater than 0 degrees and less than 90 degrees;

b. providing a means of rotating said birefringent crystal,

whereby a time delay between said two orthogonally polarized laser pulses that travel through said rotational delay crystal can be continually adjusted by rotating said rotational delay crystal about its surface normal.

12. The method of claim 11, wherein said flat birefringent crystal is selected from the group consisting of calcite crystal, quartz crystal, alpha-barium borate (alpha-BBO) crystal, and yttrium orthovanadate (YVO4) crystal.

13. The method of claim 11 further comprising, rotating by 180 degrees about its surface normal and attaching to said first birefringent crystal, a second identical birefringent crystal.