A Set of high Power microwave heating system was established by the authors,which could be used in joining of ceramic materials. The key part of the system is its single-mode resonant cavity. The behaviour of heating...A Set of high Power microwave heating system was established by the authors,which could be used in joining of ceramic materials. The key part of the system is its single-mode resonant cavity. The behaviour of heating materials is largely depend on the characteristics of resonant cavity, dielectric loss of materials, geometric factors of sample and incident microwave power. In order to better understand and control the heating process of dielectric materials bonding, numerical analysis of the heating processes of AL2O3 and Si3N4 ceramics heated in a TE10n single mode cavity was performed and some results useful for making practical heating procedures were obtained.展开更多
We propose a scheme to implement a two-qubit conditional quantum phase gate via a single mode cavity and a cascade four-level atom assisted by a classical laser. The quantum information is encoded.on the Flock states ...We propose a scheme to implement a two-qubit conditional quantum phase gate via a single mode cavity and a cascade four-level atom assisted by a classical laser. The quantum information is encoded.on the Flock states of the cavity mode and the two metastable ground states of the atom. Even under the condition of systematic dissipations, this scheme can also be realized with fidelity of 98.6% and success probability of 0.767.展开更多
We propose a scheme to implement two-qubit controlled quantum phase gate（CQPG） via a single trapped two-level ion located in the standing wave field of a quantum cavlty, in which the trap works beyond the Lamb--Dick...We propose a scheme to implement two-qubit controlled quantum phase gate（CQPG） via a single trapped two-level ion located in the standing wave field of a quantum cavlty, in which the trap works beyond the Lamb--Dicke limit. When the light field is resonant with the atomic transition ｜g） →← ｜e） of the ion located at the antinode of the standing wave, we can perform CQPG between the internal and external states of the trapped ion; while the frequency of the light field is chosen to be resonant with the first red sideband of the collective vibrational mode of the ion located at the node of the standing wave, we can perform CQPG between the cavity mode and the collective vibrational mode of the trapped ion. Neither the Lamb--Dicke approximation nor the assistant classical laser is needed. Also we can generate a GHZ state if assisted with a classical laser.展开更多
文摘A Set of high Power microwave heating system was established by the authors,which could be used in joining of ceramic materials. The key part of the system is its single-mode resonant cavity. The behaviour of heating materials is largely depend on the characteristics of resonant cavity, dielectric loss of materials, geometric factors of sample and incident microwave power. In order to better understand and control the heating process of dielectric materials bonding, numerical analysis of the heating processes of AL2O3 and Si3N4 ceramics heated in a TE10n single mode cavity was performed and some results useful for making practical heating procedures were obtained.
基金The project supported by National Natural Science Foundation of China under Grant No. 10374025
文摘We propose a scheme to implement a two-qubit conditional quantum phase gate via a single mode cavity and a cascade four-level atom assisted by a classical laser. The quantum information is encoded.on the Flock states of the cavity mode and the two metastable ground states of the atom. Even under the condition of systematic dissipations, this scheme can also be realized with fidelity of 98.6% and success probability of 0.767.
基金Project supported by the National Natural Science Foundation of China （Grant No 10374025）.
文摘We propose a scheme to implement two-qubit controlled quantum phase gate（CQPG） via a single trapped two-level ion located in the standing wave field of a quantum cavlty, in which the trap works beyond the Lamb--Dicke limit. When the light field is resonant with the atomic transition ｜g） →← ｜e） of the ion located at the antinode of the standing wave, we can perform CQPG between the internal and external states of the trapped ion; while the frequency of the light field is chosen to be resonant with the first red sideband of the collective vibrational mode of the ion located at the node of the standing wave, we can perform CQPG between the cavity mode and the collective vibrational mode of the trapped ion. Neither the Lamb--Dicke approximation nor the assistant classical laser is needed. Also we can generate a GHZ state if assisted with a classical laser.
