An energetic material device is disclosed. The energetic material device can include a casing. The energetic material device can also include an energetic material in a solid state within the casing. In addition, the energetic material device can include an optical sensor encased within the energetic material to sense a condition of the energetic material. An energetic material monitoring system is also disclosed. The energetic material monitoring system can include an energetic material device. The energetic material device can include a casing. The energetic material device can also include an energetic material in a solid state within the casing. In addition, the energetic material device can include an optical sensor encased within the energetic material. The energetic material monitoring system can also include an interrogator in communication with the optical sensor via an optical fiber.

A composed multicore optical fiber (MCF) device includes a first segment (MCF1) of a MCF having three coupled identical cores and having a first length (L1) and a second segment (MCF2) of the same MCF having a second length (L2). L1 and L2 are different from each other. One of the three coupled cores is located in a geometrical centre of the MCF. The first segment (MCF1) and the second segment (MCF2) of the MCF are rotated 180° relative to each other and spliced together. The first segment (MCF1) is spliced to a first segment (SMF1) of a single mode fiber (SMF) and the second segment (MCF2) is spliced to a second segment (SMF2) of the SMF. The free end of the second segment (SMF2) of the SMF is coupled to a mirror (M) to reflect an optical signal coming from the first segment (SMF1) of the SMF.

A watch including a watch case, wherein the watch case includes a device for measuring the degree of humidity inside the watch, wherein the device for measuring the degree of humidity is a fibre optic device including a measuring optical fibre, the measuring optical fibre includes a portion configured such that the refractive index of said portion changes in the presence of water vapour inside the watch case.

An optical sensor having one or more sensing interference elements is disclosed. A first detector function generates a coarse optical path difference signal for example using a discrete Fourier transform of a detected interference spectrum, and a second detector function generates a refined optical path difference signal using the coarse optical path difference signal and for example a cross correlation of the interference spectrum with one or more sets of periodic transfer functions.

Systems and methods for an integrated optical atomic sensor are provided. In one embodiment, an optical atomic sensor comprises: first and second photonic integrated circuits and an atom trapping chamber positioned between and bonded to the photonic integrated circuits with the integrated circuits aligned parallel to each other; and atomic vapor sealed within the chamber; wherein the first and second photonic integrated circuits each comprise: a plurality of grating emitters fabricated into respective surfaces of the first and second photonic integrated circuits waveguides configured to couple laser light from laser light sources to the grating emitters; wherein at least one set of the grating emitters are arranged to launch laser light beams into the chamber in a pattern structured to cool the vapor and produce at least one atom trap; wherein the grating emitters further include at least one grating emitter configured to emit a laser light probe into vapor.

Systems and methods of signal processing for sensors are disclosed. Signal processing methods and systems demodulate the optical interference phase of cascaded individual optical fiber intrinsic Fabry-Perot interferometric sensors in a coherent microwave-photonic interferometry distributed sensing system. The chirp effect of an electro-optic modulator (EOM) is used to create a quasi-quadrature optical interference phase shift between two adjacent pulses which correspond to two adjacent reflection points in the time domain. The phase shift can be controlled by adjusting the bias voltage that is applied to the EOM. The interference phase is calculated by elliptically fitting the phase shift. The interference phase change is proportional to the optical path difference (OPD) change of the interferometer, and the sign can be used to differentiate the increase or decrease of the OPD. The approach shows good linearity, high resolution, and large dynamic range for distributed strain sensing.

An energetic material device is disclosed. The energetic material device can include a casing. The energetic material device can also include an energetic material in a solid state within the casing. In addition, the energetic material device can include an optical sensor encased within the energetic material to sense a condition of the energetic material. An energetic material monitoring system is also disclosed. The energetic material monitoring system can include an energetic material device. The energetic material device can include a casing. The energetic material device can also include an energetic material in a solid state within the casing. In addition, the energetic material device can include an optical sensor encased within the energetic material. The energetic material monitoring system can also include an interrogator in communication with the optical sensor via an optical fiber.

A self-delayed homodyne interferometer includes light source unit, a splitting unit, an interference signal acquisition unit, a scattered light intensity acquisition unit, and a signal processing unit. The light source unit generates probe light. The splitting unit splits into two branches, Brillouin backscattered light occurring in an optical fiber to be measured with the probe light. The acquisition unit receives scattered light of one branch, and uses a self-delayed homodyne interferometer to generate an interference signal. The acquisition unit receives scattered light of the other branch, and acquires intensity of the scattered light. The signal processing unit separates and acquires a frequency shift amount from the intensity of the interference signal, and strain and temperature change from the intensity of the scattered light. The acquisition unit can change a phase of the scattered light of the one of the two branches.

Systems and methods for an integrated optical atomic sensor are provided. In one embodiment, an optical atomic sensor comprises: first and second photonic integrated circuits and an atom trapping chamber positioned between and bonded to the photonic integrated circuits with the integrated circuits aligned parallel to each other; and atomic vapor sealed within the chamber; wherein the first and second photonic integrated circuits each comprise: a plurality of grating emitters fabricated into respective surfaces of the first and second photonic integrated circuits waveguides configured to couple laser light from laser light sources to the grating emitters; wherein at least one set of the grating emitters are arranged to launch laser light beams into the chamber in a pattern structured to cool the vapor and produce at least one atom trap; wherein the grating emitters further include at least one grating emitter configured to emit a laser light probe into vapor.

An optical sensor having one or more sensing interference elements is disclosed. A first detector function generates a coarse optical path difference signal for example using a discrete Fourier transform of a detected interference spectrum, and a second detector function generates a refined optical path difference signal using the coarse optical path difference signal and for example a cross correlation of the interference spectrum with one or more sets of periodic transfer functions.