Aspects of the present disclosure describe techniques for mitigating charging on optical windows. For example, a device for mitigating charges inside a chamber of a trapped ion system is described that includes an array of parallel wires formed from a single, conductive plate by cutting elongated gaps through an entire thickness of the conductive plate that separate the wires, an outer portion of the conductive plate to which the wires are attached is configured to position the wires to run parallel to one or more trapped ions in the chamber and to position the wires between a dielectric component of the chamber and the one or more trapped ions. A chamber with such an array of parallel wires and a method of using such an array of parallel wires are also described.

The disclosure provides an atomic object trap apparatus and a method of operating such. The atomic object trap apparatus comprises two or more radio frequency (RF) electrodes formed concentrically in a substantially elliptical shape; and three or more trapping and/or transport (TT) electrode sequences formed concentrically in a substantially elliptical shape. The two or more RF electrodes and the three or more TT electrode sequences define a substantially elliptically-shaped atomic object trap. At least one TT electrode sequence of the three or more TT electrode sequences is disposed concentrically between the two or more RF electrodes. Each RF electrode and TT electrode sequence is elliptically shaped such that each comprises two substantially parallel longitudinal regions and two arc-spanning beltway regions, the four regions forming a substantially elliptical shape. The method is directed to operating a quantum computing system comprising an example atomic object trap apparatus.

A device for controlling trapped ions includes a substrate. An electrode structure is mounted on the substrate. The electrode structure includes DC electrodes and RF electrodes of an ion trap configured to trap ions in a space above the substrate. A temperature sensor is disposed at the substrate and configured to sense temperatures below 50K.

The disclosure describes aspects of using multiple species in trapped-ion nodes for quantum networking. In an aspect, a quantum networking node is described that includes multiple memory qubits, each memory qubit being based on a .sup.171Yb.sup.+ atomic ion, and one or more communication qubits, each communication qubit being based on a .sup.138Ba.sup.+ atomic ion. The memory and communication qubits are part of a lattice in an atomic ion trap. In another aspect, a quantum computing system having a modular optical architecture is described that includes multiple quantum networking nodes, each quantum networking node including multiple memory qubits (e.g., based on a .sup.171Yb.sup.+ atomic ion) and one or more communication qubits (e.g., based on a .sup.138Ba.sup.+ atomic ion). The memory and communication qubits are part of a lattice in an atomic ion trap. The system further includes a photonic entangler coupled to each of the multiple quantum networking nodes.

In one aspect, a method of performing mass spectrometry is disclosed, which comprises ionizing a sample to generate a plurality of precursor ions, passing the precursor ions through a mass filter to select at least one subset of the ions, introducing the selected ions into a branched radiofrequency (RF) ion trap and subjecting at least a portion of said selected precursor ions to fragmentation within the ion trap so as to generate a first plurality of fragment ions. The method can further include isolating at least a portion of the first plurality of fragment ions in at least one branch of the branched RF ion trap, removing unwanted fragment ions, releasing the remaining ions from said at least one branch and subjecting at least a portion thereof to fragmentation so as to generate a second plurality of fragment ions. Any combination of collision induced dissociation (CID) and electron activation dissociation (EAD) can be employed for fragmenting the ions.

The disclosure describes aspects of using multiple species in trapped-ion nodes for quantum networking. In an aspect, a quantum networking node is described that includes multiple memory qubits, each memory qubit being based on a .sup.171Yb.sup.+ atomic ion, and one or more communication qubits, each communication qubit being based on a .sup.138Ba.sup.+ atomic ion. The memory and communication qubits are part of a lattice in an atomic ion trap. In another aspect, a quantum computing system having a modular optical architecture is described that includes multiple quantum networking nodes, each quantum networking node including multiple memory qubits (e.g., based on a .sup.171Yb.sup.+ atomic ion) and one or more communication qubits (e.g., based on a .sup.138Ba.sup.+ atomic ion). The memory and communication qubits are part of a lattice in an atomic ion trap. The system further includes a photonic entangler coupled to each of the multiple quantum networking nodes.

Aspects of the present disclosure describe techniques for optical alignment using a reflective dove prism. For example, a system for optical alignment is described that includes an assembly having a housing with three separate, reflecting structures positioned to produce three reflections of one or more laser beams or one or more images, and a controller configured to control a rotation of the assembly about a pivot point to produce a tilt in orientation of the one or more lasers beams or the one or more images that is twice an angle of rotation of the assembly. Another system and a method for aligning laser beams using a housing with three separate, reflecting structures in a trapped ion quantum information processing (QIP) system are also described.

A mass spectrometric system comprises an RF-device for transversely confining ions in an ion region using: (a) a first set of electrodes arranged parallel to one another along a direction of ion travel to define a first transverse boundary of the ion region, and that are supplied with a first RF-voltage such that opposite phases of the first RF-voltage are applied to adjacent electrodes of the first set; and (b) a second set of electrodes arranged parallel to one another along said direction of ion travel to define a second transverse boundary of the ion region, and that are supplied with a second RF-voltage such that opposite phases of the second RF-voltage are applied to adjacent electrodes of the second set, the first and second transverse boundaries being opposite each other in a transverse direction of the ion region and the first and second RF voltages having different frequencies.

The invention relates to a mass spectrometer, a mass spectrometry method and a detection system. The mass spectrometer includes a vacuum chamber having a working pressure being 0.1 Pa≤P≤10 Pa; a linear ion trap, arranged in the vacuum chamber, wherein a field radius r of the linear ion trap is r≤5 mm; and a power supply, configured to provide a radio-frequency voltage for the linear ion trap, a frequency f of the radio-frequency voltage being 2 MHz≤f≤10 MHz. Because a vacuum level is relatively low, this vacuum condition may be realized by selecting a roughing pump for evacuating; and compared with a combined pump unit which is generally selected by a traditional mass spectrometer using the linear ion trap and is composed of a turbo molecular pump and a roughing pump, the roughing pump has a lower pumping speed, smaller size and lower manufacturing cost.

In order to simplify a power circuit, a linear ion trap (2) according to the present invention includes: two first rod electrodes (21, 22) facing each other across a central axis (C), each of the first rod electrodes having an opening (21a, 22a); two second rod electrodes (23, 24) facing each other across the central axis, in a direction different from the direction in which the two first rod electrodes face each other; and a pair of end electrodes (25, 26) respectively arranged outside the two end faces of the two first rod electrodes and the two second rod electrodes. A controller (7) is provided to control a radio-frequency voltage supplier (4) which applies a radio-frequency voltage for capturing ions to each of the two second rod electrodes, and an excitation voltage supplier (5) which applies a voltage for resonance excitation to each of the two first rod electrodes.