Quasi-achromatic optical isolators and circulators

Claim 2

A quasi-achromatic optical isolator having first and second ports between which a light beam may propagate, comprising: a first plane polarizer adjacent said first port of said isolator: two or more nonreciprocal optical rotators; two or more linearly birefringent plates; and a second plane polarizer adjacent said second port of said isolator: said nonreciprocal optical rotators and said linearly birefringent plates being positioned in alternating sequence between said first and second plane polarizers.

Claim 3

The optical isolator of claim 1 wherein said nonreciprocal optical rotators have a rotation angle of 45 degrees or an integral multiple thereof at a nominal center wavelength and at a nominal operating temperature.

Claim 4

The optical isolator of claim 2 wherein over a wavelength range about said nominal center wavelength: a light beam entering said first port is unattenuated by said second polarizer upon exiting said second port: and a light beam entering said second port is strongly attenuated by said first polarizer upon exiting through said first port.

Claim 5

The optical isolator of claim 1 wherein said nonreciprocal optical rotators are Faraday rotators composed of the same material such that they have exactly proportional wavelength and temperature dependencies, thereby compensating for wavelength changes and temperature variations.

Claim 6

A quasi-achromatic optical isolator through which a light beam within a wavelength range about a nominal wavelength may propagate along a +z coordinate axis comprising: a first plane polarizer accepting said light beam at a first port and transmitting said light beam polarized along an orthogonal x coordinate axis; a first Faraday rotator receiving said light beam which has passed through said first plane polarizer; a first linearly birefringent plate oriented with its fast axis along the x axis and receiving said light beam which has passed through said first Faraday rotator; a second Faraday rotator receiving said light beam which has passed through said first linearly birefringent plate; a second linearly birefringent plate oriented with its fast axis along the x axis and receiving said light beam which has passed through said second Faraday rotator; a second plane polarizer receiving the light beam which has passed through said second linearly birefringent plate, transmitting said light beam undiminished in intensity, and exiting said light beam at a second port.

Claim 7

A quasi-achromatic optical isolator through which a light beam within a wavelength range about a nominal wavelength may propagate along a +z coordinate axis comprising: a first plane polarizer accepting said light beam at a first port and transmitting said light beam polarized along an orthogonal x coordinate axis; a first Faraday rotator receiving said light beam which has passed through said first plane polarizer; a first linearly birefringent plate oriented with its fast axis along the x axis and receiving said light beam which has passed through said first Faraday rotator; a second Faraday rotator receiving said light beam which has passed through said first linearly birefringent plate; a second linearly birefringent plate oriented with its fast axis along the x axis and receiving said light beam which has passed through said second Faraday rotator; a second plane polarizer receiving the light beam which has passed through said second linearly birefringent plate, transmitting said light beam undiminished in intensity, and exiting said light beam at a second port.

Claim 8

The optical isolator of claim 5 wherein: said first Faraday rotator has a rotation angle of +n degrees; and said second Faraday rotator has a rotation angle of +2n degrees.

Claim 9

The optical isolator of claim 6 wherein said first and said second linearly birefringent plates have +120 degrees of retardation.

Claim 10

The optical isolator of claim 6 wherein said first and said second linearly birefringent plates have -120 degrees of retardation.

Claim 11

The optical isolator of claim 5 wherein: said first Faraday rotator has a rotation angle of +n degrees; and said second Faraday rotator has a rotation angle of -2n degrees.

Claim 12

The optical isolator of claim 9 wherein said first and said second linearly birefringent plates have +60 degrees of retardation.

Claim 13

The optical isolator of claim 9 wherein said first and said second linearly birefringent plates have -60 degrees of retardation.

Claim 14

The optical isolator of claim 6 or 9 wherein: n=+45 degrees at said nominal wavelength; and the orientation of the polarization axis of said second plane polarizer is equal to -45 degrees.

Claim 15

The optical isolator of claim 6 or 9 wherein: n=-45 degrees at said nominal wavelength; and the orientation of the polarization axis of said second plane polarizer is equal to +45 degrees.

Claim 16

The optical isolator of claim 5 wherein said Faraday rotators are composed of the same material such that they have exactly proportional wavelength and temperature dependencies, thereby compensating for wavelength changes and temperature variations.

Claim 17

The optical isolator of claim 14 wherein the Faraday rotators comprise crystals of yttrium iron garnet.

Claim 18

The optical isolator of claim 5 wherein said birefringent plates are constructed for said nominal wavelength equal to 1.42 microns.

Claim 19

A quasi-achromatic optical isolator through which a light beam within a wavelength range about a nominal wavelength may propagate along a +z coordinate axis comprising: a first plane polarizer accepting said light beam at a first port and transmitting said light beam polarized along an orthogonal x coordinate axis; a first Faraday rotator receiving the light beam which has passed through said first plane polarizer; a first plurality of linearly birefringent plates receiving the light beam which has passed through said first Faraday rotator; a second Faraday rotator receiving the light beam which has passed through said first plurality of linearly birefringent plates; a second plurality of linearly birefringent plates receiving the light beam which has passed through the second Faraday rotator; a second plane polarizer receiving the light beam which has passed through said second plurality of linearly birefringent plates, transmitting said light beam undiminished in intensity, and exiting said light beam at a second port.

Claim 20

A quasi-achromatic optical isolator through which a light beam within a wavelength range about a nominal wavelength may propagate along a +z coordinate axis comprising: a first plane polarizer accepting said light beam at a first port and transmitting said light beam polarized along an orthogonal x coordinate axis; a first Faraday rotator receiving the light beam which has passed through said first plane polarizer; a first plurality of linearly birefringent plates receiving the light beam which has passed through said first Faraday rotator; a second Faraday rotator receiving the light beam which has passed through said first plurality of linearly birefringent plates; a second plurality of linearly birefringent plates receiving the light beam which has passed through the second Faraday rotator; a second plane polarizer receiving the light beam which has passed through said second plurality of linearly birefringent plates, transmitting said light beam undiminished in intensity, and exiting said light beam at a second port.

Claim 21

The optical isolator of claim 17 wherein: said first Faraday rotator has a rotation angle of +n degrees; and said second Faraday rotator has a rotation angle of +2n degrees.

Claim 22

The optical isolator of claim 18 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between +116 and +120 degrees.

Claim 23

The optical isolator of claim 18 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between -116 and -120 degrees.

Claim 24

The optical isolator of claim 17 wherein: said first Faraday rotator has a rotation angle of +n degrees: and said second Faraday rotator has a rotation angle of -2n degrees.

Claim 25

The optical isolator of claim 21 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between +60 and +64 degrees.

Claim 26

The optical isolator of claim 21 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between -60 and -64 degrees.

Claim 27

The optical isolator of claim 18 or 21 wherein n=+45 degrees at said nominal wavelength.

Claim 28

The optical isolator of claim 18 or 21 wherein n=-45 degrees at said nominal wavelength.

Claim 29

The optical isolator of claim 18 or 21 wherein the orientation of the polarization axis of said second plane polarizer is equal to 90 degrees.

Claim 30

The optical isolator of claim 18 or 21 wherein the orientation of the polarization axis of said second plane polarizer is equal to zero degrees.

Claim 31

The optical isolator of claim 17 wherein the transmission in the forward direction from said first port to said second port and the isolation in the reverse direction from said second port to said first port are optimized at two wavelengths oppositely displaced from said nominal wavelength.

Claim 32

The optical isolator of claim 17 wherein said second plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength for converting elliptically polarized light from said second Faraday rotator to plane polarized light for transmission by said second polarizer.

Claim 33

The optical isolator of claim 17 wherein said Faraday rotators are composed of the same material such that they have exactly proportional wavelength and temperature dependencies, thereby compensating for wavelength changes and temperature variations.

Claim 34

A quasi-achromatic optical circulator having first, second, third, and fourth ports comprising: a first polarizing beam splitter adjacent said first and said third ports of said circulator; two or more nonreciprocal optical rotators; two or more linearly birefringent plates; a second polarizing beam splitter adjacent said second and said fourth ports of said circulator; and said nonreciprocal optical rotators and said linearly birefringent plates being positioned in alternating sequence between said first and second polarizing beam splitters; whereby light entering said first port is directed to said second port; light entering said second port is directed to said third port; light entering said third port is directed to said fourth port; and light entering said fourth port is directed to said first port.

Claim 35

A quasi-achromatic optical circulator having first, second, third, and fourth ports comprising: a first polarizing beam splitter adjacent said first and said third ports of said circulator; two or more nonreciprocal optical rotators; two or more linearly birefringent plates; a second polarizing beam splitter adjacent said second and said fourth ports of said circulator; and said nonreciprocal optical rotators and said linearly birefringent plates being positioned in alternating sequence between said first and second polarizing beam splitters; whereby light entering said first port is directed to said second port; light entering said second port is directed to said third port; light entering said third port is directed to said fourth port; and light entering said fourth port is directed to said first port.

Claim 36

The optical circulator of claim 31 wherein said nonreciprocal optical rotators are Faraday rotators having a rotation angle of 45 degrees or an integral multiple thereof at a nominal center wavelength and at a nominal operating temperature.

Claim 37

A quasi-achromatic optical circulator having first, second, third, and fourth ports that may accept a light beam within a wavelength range about a nominal wavelength and direct it to a succeeding port and comprising: a first polarizing beam splitter adjacent said first and said third ports of said circulator; a first Faraday rotator receiving a light beam which has passed through said first polarizing beam splitter; a first plurality of linearly birefringent plates receiving the light beam which has passed through said first Faraday rotator: a second Faraday rotator receiving the light beam which has passed through said first plurality of linearly birefringent plates; a second plurality of linearly birefringent plates receiving the light beam which has passed through said second Faraday rotator: and a second polarizing beam splitter adjacent said second and said fourth ports of said circulator for receiving the light beam which has passed through said second plurality of linearly birefringent plates and directing said light beam undiminished in intensity to said succeeding port.

Claim 38

A quasi-achromatic optical circulator having first, second, third, and fourth ports that may accept a light beam within a wavelength range about a nominal wavelength and direct it to a succeeding port and comprising: a first polarizing beam splitter adjacent said first and said third ports of said circulator; a first Faraday rotator receiving a light beam which has passed through said first polarizing beam splitter; a first plurality of linearly birefringent plates receiving the light beam which has passed through said first Faraday rotator: a second Faraday rotator receiving the light beam which has passed through said first plurality of linearly birefringent plates; a second plurality of linearly birefringent plates receiving the light beam which has passed through said second Faraday rotator: and a second polarizing beam splitter adjacent said second and said fourth ports of said circulator for receiving the light beam which has passed through said second plurality of linearly birefringent plates and directing said light beam undiminished in intensity to said succeeding port.

Claim 39

The optical circulator of claim 33 wherein the orientations of the polarization axes of said first polarizing beam splitter are equal to 0 and 90 degrees.

Claim 40

The optical circulator of claim 36 wherein: said first Faraday rotator has a rotation angle of +n degrees; and said second Faraday rotator has a rotation angle of +2n degrees.

Claim 41

The optical circulator of claim 35 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between +116 and +120 degrees.

Claim 42

The optical circulator of claim 35 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between -116 and -120 degrees.

Claim 43

The optical circulator of claim 34 wherein: said first Faraday rotator has a rotation angle of +n degrees; and said second Faraday rotator has a rotation angle of -2n degrees.

Claim 44

The optical circulator of claim 38 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between +60 and +64 degrees.

Claim 45

The optical circulator of claim 38 wherein said first plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength and equivalent to an optical rotator followed by a linear retardation between -60 and -64 degrees.

Claim 46

The optical circulator of claim 35 or 38 wherein n=+45 degrees at said nominal wavelength.

Claim 47

The optical circulator of claim 35 or 38 wherein n=-45 degrees at said nominal wavelength.

Claim 48

The optical circulator of claim 34 wherein the orientations of the polarization axes of said second polarizing beam splitter are equal to 0 and 90 degrees.

Claim 49

The optical circulator of claim 33 wherein the transmission in the forward direction between succeeding ports and the isolations between non succeeding ports are optimized at two wavelengths symmetrically displaced from said nominal wavelength.

Claim 50

The optical circulator of claim 33 wherein said second plurality of linearly birefringent plates constitutes a combination plate quasi-achromatic about said nominal wavelength for converting elliptically polarized light from said second Faraday rotator to plane polarized light for transmission by said second polarizer.