A system for atom interferometry includes one or more lasers disposed to 1) generate a first pair of beams that are initially spatially separated and later overlapped to follow a common path to intersecting an atomic cloud interaction region, wherein the first beam of the pair of beams acts as a first MOT beam and the second beam of the pair of beams acts as a first Raman beam; and 2) generate an additional beam, wherein the additional beam is multiplexed to be used alternately as a second MOT beam and as a second Raman beam, wherein the additional beam follows an opposing path to the common path when intersecting the atomic cloud interaction region.

A system for atom interferometry includes one or more lasers disposed to 1) generate a first pair of beams that are initially spatially separated and later overlapped to follow a common path to intersecting an atomic cloud interaction region, wherein the first beam of the pair of beams acts as a first MOT beam and the second beam of the pair of beams acts as a first Raman beam; and 2) generate an additional beam, wherein the additional beam is multiplexed to be used alternately as a second MOT beam and as a second Raman beam, wherein the additional beam follows an opposing path to the common path when intersecting the atomic cloud interaction region.

An attitude sensor system with automatic bias correction having a primary attitude sensor wherein the primary attitude sensor comprises at least one accelerometer and an auxiliary sensor system configured to automatically estimate a bias of the accelerometer of the primary attitude sensor such that the resulting error is removed from an output of the attitude sensor system.

Systems and methods are disclosed for deriving linear acceleration using an accelerometer. The orientation of a device may be determined using only accelerometer data. The determined orientation may then be used to determine a gravity vector, such that linear acceleration may be derived by subtracting the gravity vector from accelerometer data.

Systems and methods are disclosed for deriving linear acceleration using an accelerometer. The orientation of a device may be determined using only accelerometer data. The determined orientation may then be used to determine a gravity vector, such that linear acceleration may be derived by subtracting the gravity vector from accelerometer data.

A lens module includes a lens, a first gravity sensor and a processor. The lens includes an optical axis and an adjustment assembly. The adjustment assembly rotates around the optical axis. The first gravity sensor is disposed on the adjustment assembly. The adjustment assembly drives the first gravity sensor to rotate. The first gravity sensor is configured to perform detection at different time points. The first gravity sensor generates a first output at a first time point and a second output at a second time point. The processor calculates first and second angles of the first gravity sensor relative to a water level according to the first and second outputs respectively. The processor controls a focus adjustment of the lens according to the first angle and the second angle. A projector employing the aforementioned lens module is also provided.

A lens module includes a lens, a first gravity sensor and a processor. The lens includes an optical axis and an adjustment assembly. The adjustment assembly rotates around the optical axis. The first gravity sensor is disposed on the adjustment assembly. The adjustment assembly drives the first gravity sensor to rotate. The first gravity sensor is configured to perform detection at different time points. The first gravity sensor generates a first output at a first time point and a second output at a second time point. The processor calculates first and second angles of the first gravity sensor relative to a water level according to the first and second outputs respectively. The processor controls a focus adjustment of the lens according to the first angle and the second angle. A projector employing the aforementioned lens module is also provided.

The disclosure provides a diamagnetically stabilized magnetically levitated gravimeter and related method that allows measurements of relative gravity in a simple, low power consumption device based on a magnetic levitation principle using permanent magnets instead of using a mechanical spring. The gravimeter uses magnetic forces to balance a float magnet against the force of gravity, allowing for accurate measurements. The gravimeter includes a float magnet that floats between two diamagnetic materials, such as diamagnetic plates, without a need for external energy input due to the interaction between the magnetic forces of the float magnet lifted by the lift magnet but stabilized between upper and lower diamagnetic materials. The gravimeter is less sensitive to drift in response to stresses than a mechanical spring, have a lower temperature sensitivity, and lower energy and power requirements to take similarly reliable gravity measurements, which in turn simplify deployment and prolong operational lifetime.

The disclosure provides a diamagnetically stabilized magnetically levitated gravimeter and related method that allows measurements of relative gravity in a simple, low power consumption device based on a magnetic levitation principle using permanent magnets instead of using a mechanical spring. The gravimeter uses magnetic forces to balance a float magnet against the force of gravity, allowing for accurate measurements. The gravimeter includes a float magnet that floats between two diamagnetic materials, such as diamagnetic plates, without a need for external energy input due to the interaction between the magnetic forces of the float magnet lifted by the lift magnet but stabilized between upper and lower diamagnetic materials. The gravimeter is less sensitive to drift in response to stresses than a mechanical spring, have a lower temperature sensitivity, and lower energy and power requirements to take similarly reliable gravity measurements, which in turn simplify deployment and prolong operational lifetime.

A system for atom interferometry includes one laser configured to generate an output beam; an acousto-optic deflector disposed to generate two diffracted beams that are spatially offset with identical polarizations; and a birefringent crystal disposed to receive the two diffracted beams, where one of the two diffracted beams is passed through a half wave plate so that the two diffracted beams have orthogonal polarizations, where the birefringent crystal further disposed and selected in size to enable the two diffracted beams to re-overlap upon exiting the birefringent crystal by having one of the two diffracted beams walk toward the other of the two diffracted beams in the birefringent crystal, where the two diffracted beams have minimal path length differences so that the two diffracted beams are useable for interferometry.