The driver condition detection system includes a driver monitor camera capturing a face of a driver of a vehicle and generating a facial image of the driver, and a driver condition detection part configured to detect a condition of the driver based on the facial image. If a part of face parts of the driver is hidden in the facial image, the driver condition detection part is configured to detect a condition of the driver based on face parts of the driver not hidden in the facial image. The face parts of the driver are a mouth, nose, right eye, and left eye of the driver.

An ion optical device includes one or more pairs of confinement electrode units arranged at two sides of a first direction; a power supply device for applying opposite radio-frequency voltages to the paired confinement electrode units respectively and forming thereon DC potentials distributed in a second direction orthogonal to the first direction to form a potential barrier herein over a length portion of the first direction; one first area and one second area positioned at two sides of the potential barrier in the second direction; and a control device connected with the power supply device for controlling an output thereof to change the potential barrier to manipulate the ions transported/stored in the first area being transferred to the second area through the potential barrier in ways based on the mass to charge ratio or mobility of the ions and continue being transported along the first direction.

A ring stacked accelerator for use in a mass spectrometer includes a plurality of ring shaped plates arranged in a stack and is electrically coupled to a voltage divider that allows a substantially homogeneous electric field to be produced when the stack is energized. The voltage divider can include resistors and capacitors, where the capacitors are chosen to compensate for parasitic capacitances experienced by the plates. The ring stacked accelerator can be energized using an RF pulse. The ring stack accelerator can include one or more balancing capacitors for correcting effects that cause nonlinearity.

A Time of Flight mass spectrometer is disclosed wherein a fifth order spatial focusing device is provided. The device which may comprise an additional stage in the source region of the Time of Flight mass analyser is arranged to introduce a non-zero fifth order spatial focusing term so that the combined effect of first, third and fifth order spatial focusing terms results in a reduction in the spread of ion arrival times T of ions arriving at the ion detector.

A mass spectrometer comprising: a pulsed ion source for generating pulses of ions having a range of masses; a time-of-flight mass analyzer for receiving and mass analyzing the pulses of ions from the ion source; and an energy controlling electrode assembly located between the pulsed ion source and the time-of-flight mass analyzer configured to receive the pulses of ions from the pulsed ion source and apply a time-dependent potential to the ions thereby to control the energy of the ions depending on their m/z before they reach the time-of-flight mass analyzer. Mass dependent differences in average energy of ions can be reduced for injection into a time-of-flight mass analyzer, which can improve ion transmission and/or instrument resolving power.

The present invention provides a time-of-flight mass spectrometer (TOFMS) taken measures for preventing a deterioration in accuracy caused at the time of transportation to an installation site. A time-of-flight mass spectrometer (TOFMS) for performing mass separation based on the time of flight of an ion flying in a flight space includes an ion transportation unit (12, 14, 15) configured to transport an ion, an acceleration unit (expulsion electrode (161) and the like) configured to receive the ion transported by the ion transportation unit and accelerate the ion to introduce the ion into the flight space, a flight unit incorporating the flight space, a first vacuum vessel (18A) enclosing the ion transportation unit, the acceleration unit, and at least a part of the flight unit, a chassis (19) on which the first vacuum vessel (18A) is placed, and a reflector unit (20) to which a reflector (reflection (164)) and a second vacuum vessel (28) are fixed, the reflection (164) being configured to reverse the flight trajectory of the ion accelerated by the acceleration unit and introduced into the flight space, and the second vacuum vessel (28) being attachable to an end of the first vacuum vessel (18A) and enclosing the reflector. Since the reflector unit (20) is separated from other parts during transportation, the other parts are easily moved by, for example, casters (191) disposed on the chassis (19), and the reflector unit (20) is moved without being affected by the vibrations caused by the movement on the casters (191).

The invention relates to a mass spectrometer with laser-desorption ion source, particularly for MALDI. A laser system with optical laser spot control is proposed in which the laser spot shift brought about by means of a temporally variable angular deflection at a mirror system is performed on the laser beam before or during the energy multiplication. The laser beam, which is deflected through a small angle by the mirror system, is converted by a suitable flat-field optical system into a parallel-shifted laser beam, which then passes through a multiplier crystal. After exiting the multiplier crystal system, the parallel-shifted beam is converted back into a slightly angled beam by a flat-field optical system, this latter beam then bringing about the spot shift on the sample. The multiplier crystal is conserved by the continuously temporally changed parallel shift of the laser beam in the multiplier crystal, thus prolonging its service life.

Elongation of orthogonal accelerators is assisted by ion spatial transverse confinement within novel confinement means, formed by spatial alternation of electrostatic quadrupolar field (22). Contrary to prior art RF confinement means, the static means provide mass independent confinement and may be readily switched. Spatial confinement defines ion beam (29) position, prevents surfaces charging, assists forming wedge and bend fields, and allows axial fields in the region of pulsed ion extraction, this way improving the ion beam admission at higher energies and the spatial focusing of ion packets in multi- reflecting, multi-turn and singly reflecting TOF MS or electrostatic traps.

A multipole ion guide (30) including a plurality of rod electrodes arranged at an angle to the central axis (C) is placed within a collision cell (13) located in the previous stage of an orthogonal accelerator (16). Radio-frequency voltages with opposite phases are applied to the rod electrodes of the ion guide (30) so that any two rod electrodes neighboring each other in the circumferential direction have opposite phases of the voltage. A depth gradient of the pseudopotential is thereby formed from the entrance end toward the exit end within the space surrounded by the rod electrodes, and ions are accelerated by this gradient. During an ion-accumulating process, a direct voltage having the same polarity as the ions is applied to the exit lens electrode (132) to form a potential barrier for accumulating ions. Among the ions repelled by the potential barrier, ions having smaller m/z return closer to the entrance end. Therefore, when the potential barrier is removed and ions are discharged, ions having smaller m/z are discharged at later points in time than those having larger m/z. Therefore, a wide m/z range of ions can be simultaneously accelerated and ejected by an orthogonal accelerator (16).

The invention relates to the operation of an energy-focusing and solid-angle-focusing reflector for time-of-flight mass spectrometers with pulsed ion acceleration into a flight tube, e.g. from an ion source with ionization by matrix-assisted laser desorption (MALDI). The objective of the invention is to generate high mass resolution in wide mass ranges up to high masses above eight kilodaltons by varying at least one operating voltage on one of the diaphragms of the reflector which can be varied according to a suitable time function during the spectrum acquisition. It may also be advantageous to adapt the operation of the accelerating voltages in the starting region of the ions accordingly. These measures make it possible to achieve a mass resolution much higher than R=100,000 in a wide mass range extending up to and above eight kilodaltons.