A method includes directing a probe beam to a target that includes an array of data portions in a data storage medium arranged so that a beam area of the probe beam extends across a plurality of adjacent data portions, the array including a data portion subset with each data portion of the subset responsive to the probe beam to produce a response illumination, receiving the response illumination at a detector, and determining data values corresponding to the plurality of adjacent data portions based on the received response illumination. Apparatus and systems are also disclosed.

A method includes directing a probe beam to a target that includes an array of data portions in a data storage medium arranged so that a beam area of the probe beam extends across a plurality of adjacent data portions, the array including a data portion subset with each data portion of the subset responsive to the probe beam to produce a response illumination, receiving the response illumination at a detector, and determining data values corresponding to the plurality of adjacent data portions based on the received response illumination. Apparatus and systems are also disclosed.

A method and apparatus to manufacture a coherent bundle of scintillating fibers is disclosed. A method includes providing a collimated bundle having a glass preform with capillaries therethrough known in the industry as a glass capillary array, and infusing the glass capillary array with a scintillating polymer or a polymer matrix containing scintillating nanoparticles.

A radiation imaging apparatus, including a plurality of pixels, a plurality of column lines and a processor, the plurality of pixels including first pixels and second pixels configured to generate signals of different values by receiving radiation rays of equal irradiation rates, and the plurality of pixels being arrayed such that their numbers are different between a first column and a second column of the plurality of columns, wherein the processor, after radiation irradiation is started, obtains a first signal of the first column and a second signal of the second column while maintaining each pixel to an OFF state and performs AEC based on the first and second signals.

A charged particle counting device, a manufacturing method thereof, and a charged particle counting system are provided. The charged particle counting device includes: a bipolar transistor (10) and a magneto-electric induction coil (20), a gate (101) of the bipolar transistor is electrically connected to an end of the magneto-electric induction coil, and the other end of the magneto-electric induction coil is applied with a constant voltage, when a stream of positively charged particles passes through the magneto-electric induction coil and a first induced voltage generated by the magneto-electric induction coil is greater than a predetermined voltage threshold, a channel of the bipolar transistor is an N-type channel; and when a stream of negatively charged particles passes through the magneto-electric induction coil and a second induced voltage generated by the magneto-electric induction coil is less than the predetermined voltage threshold, the channel of the bipolar transistor is a P-type channel.

An excitation transfer in a nuclear state is energetically induced. The excitation transfer may be induced by heating a structure to which a nuclear species is mechanically coupled. The heating may be applied as a triangular heat pulse. The heating may generate a stress effect in the structure. The stress effect may produce vibratory phonons. The excitation transfer may include up-conversion. The excitation transfer may include radioactive decay. The decay rate of a radioactive species may be increased to a rate higher than the natural half-life of the radioactive species. Energy may be harnessed from decay of the radioactive species. A decay product having industrial or medical use may be rapidly produced. The decay rate of the radioactive species may be lowered to reduce emissions for safe storage or transportation.

A method and apparatus are provided for positron emission imaging to correct a position at which a gamma ray was detected, when the gamma ray is scattered during detection. When Compton scattering occurs during detection of a gamma ray, the energy of the gamma ray deposited in multiple crystals in an array of detector elements. The corrected position is determined as a weighted sum of the position of the multiple crystals, each weighted by an inverse of the energy measured at the respective crystal. Further, the inverse-energy weight can be raised to a power p. A minimum energy threshold can be applied to determine the multiple crystals at which the gamma ray energy is deposited. The corrected position can be a floating position or can be rounded to a nearest crystal or to a nearest virtual sub-crystal.

Disclosed is a system and a method enabling the behavior of a radioactive substance within a structure to be determined. More particularly, the disclosed is a system and a method wherein it is possible to determine, along a column, the position and/or distribution and/or movement speed of the substances moving within the column and/or the time when the substances will leave the column and how much of the substance reaching the column outlet will begin to leave the column and with what activity, and consequently, it is possible to provide optimization and automation for proceeding to the next process step.

A method includes directing a probe beam to a target that includes an array of data portions in a data storage medium arranged so that a beam area of the probe beam extends across a plurality of adjacent data portions, the array including a data portion subset with each data portion of the subset responsive to the probe beam to produce a response illumination, receiving the response illumination at a detector, and determining data values corresponding to the plurality of adjacent data portions based on the received response illumination. Apparatus and systems are also disclosed.

A method and an apparatus for distinguishing radionuclides are disclosed. The method comprises the steps of: receiving energy generated in one or more radioactive elements; applying energy as a weight for each channel to spectrum of the received energy; and distinguishing the one or more radioactive elements on the basis of the spectrum of the spectrum to which the weight is applied. A radioactive element having an energy value corresponding to a peak value of the spectrum of the energy to which the weight is applied, as an energy value of a Compton edge, is distinguished as the one or more radioactive elements. According to the present invention, it is possible to more accurately monitor radiation even while using a plastic scintillator, and further to improve energy resolution of a plastic scintillator.