光学的に制御された,コヒーレントダークステートスペクトロスコピーによる核フィールドのロック
Xiaodong Xu1, Wang Yao, Bo Sun
1The H. M. Randall Laboratory of Physics, The University of Michigan, Ann Arbor, Michigan 48109, USA.
Nature
|June 26, 2009
まとめ
研究者は,量子ドットにおける核スピン変動を抑制し,電子スピン相関時間を大幅に改善しました. このブレークスルーは,新しいフィードバックプロセスを用いて,堅牢な量子論理装置の道を開く.
科学分野:
- 量子情報科学とは,量子情報科学である.
- 凝縮物質物理学 凝縮物質物理学
- 半導体スピントロニクス
背景:
- 半導体量子ドットの単一スピンは,量子コンピューティングの鍵です.
- III-V物質の核スピンは,超微細相互作用によって電子スピンの相関性を破壊する.
- 以前の方法は,核スピンの変動を抑制することに焦点を当てており,同時制御ではありませんでした.
研究 の 目的:
- 量子ドット内の単一のスピンの一貫した制御を達成し,核の変動を抑制します.
- 電子のスピンコヒーレンス時間を高める方法を示す.
- 核スピン環境の再現可能な準備を可能にするために.
主な方法:
- コヘレントダークステートスペクトロスコピーは,電子のスピン脱相時間 (T(2) *) を測定します.
- ホールスピンアシストダイナミックな核スピン極化フィードバックプロセスを利用します.
- 核フィールドのロックを実証するために3つのレーザー測定を使用します.
主要な成果:
- 核フィールドの波動は,熱値よりはるかに下まで抑制された.
- 電子スピン脱相時間 (T(2) *) は著しく増加した.
- 抑制の原因として,ホールスピン補助フィードバックメカニズムが特定されました.
- レーザーパラメータによって決定された核フィールドのロックが達成されました.
結論:
- 電子のスピン相関性を高めるための新しい,シンプルで強力な方法が開発されました.
- この技術は,複雑な"スピン・エコー"タイプの方法を避けています.
- 結果は,核環境を安定させることで,単一のスピンの再現可能な制御と測定を可能にします.
関連する概念動画
Atomic Nuclei: Nuclear Spin
5.1K
All atomic particles possess an intrinsic angular momentum, or 'spin'. Electrons, protons, and neutrons each have a spin value of ½, although protons and neutrons in nuclei may have higher half-integer spins owing to energetic factors.
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute...
Atomic nuclei have a net nuclear spin, , which can have an integer or half-integer value. In atomic nuclei, the spins of protons are paired against each other but not with neutrons, and vice versa. Consequently, an even number of protons does not contribute...
5.1K
Atomic Nuclei: Nuclear Spin State Overview
1.9K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
1.9K
Atomic Nuclei: Nuclear Spin State Population Distribution
1.7K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.7K
Atomic Nuclei: Larmor Precession Frequency
3.5K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
3.5K
Atomic Nuclei: Magnetic Resonance
1.2K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.2K
Atomic Nuclei: Nuclear Relaxation Processes
1.1K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.1K


