Pressure insensitive optical fiber

Claim 2

A pressure insensitive optical fiber waveguide comprising: a solid cylindrical light transmitting core; a cladding layer concentrically surrounding the core; substrate means concentrically surrounding the cladding layer including a layer of glass having a bulk modulus substantially higher than that of the core; said glass layer having a thickness such that external acoustic pressures thereon induce self cancelling phase shifts of light through the core; thereby rendering the waveguide substantially insensitive to environmental acoustic conditions.

Claim 3

The invention according to claim 1 further defined by a relatively soft coating concentrically surrounding the substrate.

Claim 4

A pressure insensitive optical fiber waveguide comprising: an optical fiber including an optical core and concentric cladding; a substrate concentrically surrounding the optical fiber and having a bulk modulus greater than that of the optical fiber; said substrate having a wall thickness such that external acoustic pressures thereon induce self cancelling phase shifts of light through the core; thereby rendering the waveguide insensitive to environmental acoustic conditions.

Claim 5

A pressure insensitive optical fiber waveguide comprising: an optical fiber including an optical core and concentric cladding; a substrate concentrically surrounding the optical fiber and having a bulk modulus greater than that of the optical fiber; said substrate having a wall thickness such that external acoustic pressures thereon induce self cancelling phase shifts of light through the core; thereby rendering the waveguide insensitive to environmental acoustic conditions.

Claim 6

The invention according to claim 3 further defined by the substrate wall thickness selected such that the algebraic sum of ε z l +ε r P +ε z P =0, where ##EQU6## ε z and ε r being the longitudinal and radial strain respectively of the core induced by acoustic pressure, n being the refractive index of the core, and P 11 and P 12 being the elasto-optic or Pockels coefficients of the core.

Claim 7

The invention according to claim 3 further defined by the substrate wall thickness being such that a given acoustic hydrostatic pressure exerted on the optical core cancels strains and dimension changes whereby no phase shift is induced in light passing through the core.

Claim 8

The invention according to claim 3, 4, or 5 wherein the optical core and cladding comprises K 2 O-SiO 2 .

Claim 9

The invention according to claim 6 further defined by a substrate comprising calcium aluminate.

Claim 10

The invention according to claim 6 wherein the glasses have slightly different molar ratios whereby the cladding glass has an index of refraction slightly less than that of the core glass.

Claim 11

The invention according to claim 8 wherein the molar ratios are 12-88 for the core and 10-90 for the cladding.

Claim 12

The invention according to claim 3, 4, or 5 wherein the substrate is metal.

Claim 13

The invention according to claim 10 wherein the metal is nickel.

Claim 14

A pressure insensitive optical fiber waveguide comprising; an optical fiber core and a concentrically surrounding covering; said covering having an index of refraction slightly lower than that of the core thereby defining a cladding; said covering further having a bulk modulus substantially higher than that of the core thereby further defining a substrate; said covering having a wall thickness such that acoustic pressures thereon induce mutually cancelling phase shifts in light passing through the core; thereby rendering the waveguide insensitive to acoustic pressures.

Claim 15

A pressure insensitive optical fiber waveguide comprising; an optical fiber core and a concentrically surrounding covering; said covering having an index of refraction slightly lower than that of the core thereby defining a cladding; said covering further having a bulk modulus substantially higher than that of the core thereby further defining a substrate; said covering having a wall thickness such that acoustic pressures thereon induce mutually cancelling phase shifts in light passing through the core; thereby rendering the waveguide insensitive to acoustic pressures.

Claim 16

The invention according to claim 12 wherein the substrate wall thickness is such that the algebraic sum of ε z l +ε r P +ε z P =0 where ##EQU7## ε z and ε r being the longitudinal and radial strain respectively, of the core induced by acoustic pressure, n being the refractive index of the core, and P 11 and P 12 being the elasto-optic or Pockels coefficients of the core.

Claim 17

The invention according to claim 13 further defined by the core being K 2 O-SiO 2 .

Claim 18

The invention according to claim 13 or 14 further defined by the covering being selected from the group consisting of calcium aluminate and high bulk modulus ceramic material.

Claim 19

In an optical fiber waveguide including a glass core and cladding with a glass substrate disposed concentrically about the cladding, an improved process comprising: applying an additional substrate of high bulk modulus glass concentrically about said initial glass substrate; and selecting a wall thickness for the high bulk modulus glass such that acoustic pressures thereon induce the algebraic sum of ε z l +ε r P +ε z P =0 where ##EQU8## ε z and ε r being the longitudinal and radial strain, respectively, of the core induced by acoustic pressure, n being the refractive index of the core, and P 11 and P 12 being the elasto-optic or Pockels coefficients of the core; whereby light in passing through the optical core is immune from pressure induced phase shifts.

Claim 20

In an optical fiber waveguide including a glass core and cladding with a glass substrate disposed concentrically about the cladding, an improved process comprising: applying an additional substrate of high bulk modulus glass concentrically about said initial glass substrate; and selecting a wall thickness for the high bulk modulus glass such that acoustic pressures thereon induce the algebraic sum of ε z l +ε r P +ε z P =0 where ##EQU8## ε z and ε r being the longitudinal and radial strain, respectively, of the core induced by acoustic pressure, n being the refractive index of the core, and P 11 and P 12 being the elasto-optic or Pockels coefficients of the core; whereby light in passing through the optical core is immune from pressure induced phase shifts.