相关实验视频
Updated: May 26, 2025

09:10
Fabrication and Testing of Microfluidic Optomechanical Oscillators
Published on: May 29, 2014
12.1K
洞合旋转振荡器的自主反稳定
Julian Wolf1,2, Olive H Eilbott1,2, Joshua A Isaacs1,2
1University of California, Department of Physics, Berkeley, California 94720, USA.
Physical review letters
|February 21, 2025
概括
我们使用光腔反稳定了不平衡的原子自旋组合. 这种方法允许精确控制任何能量级别的自旋状态,通过与理论预测相匹配的实验数据得到证实.
科学领域:
- 原子物理 原子物理
- 量子光学就是一个量子光学.
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 原子组合对于量子技术至关重要.
- 控制集体旋转状态是具有挑战性的,因为缺乏连贯性.
- 现有的方法通常需要特定的能量水平或复杂的设置.
研究的目的:
- 为了证明原子自旋组合的不平衡稳定.
- 为了利用自主反从驱动光学腔进行旋转控制.
- 为了在任意的能量水平上实现稳定.
主要方法:
- 采用驱动光学腔与分散合到一个原子组合.
- 将磁场应用于与腔轴的角度.
- 采用来自空腔光的连贯支持,根据空腔易感度进行条件化.
主要成果:
- 实现了集体旋转的失衡稳定.
- 对纵向和横向旋转组件都表现出敏感性.
- 在任意能量下验证了自旋状态的稳定.
- 实验结果与设定点跟踪和增益频谱的分析预测非常相匹配.
结论:
- 自主光腔反是一种稳定原子自旋组合的有效方法.
- 这种技术可以精确控制量子状态.
- 这些发现对量子信息处理和精度测量有影响.
更多相关视频
相关概念视频
Oscillations In An LC Circuit
2.2K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
2.2K
RLC Circuit as a Damped Oscillator
840
An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
840
Damped Oscillations
5.6K
In the real world, oscillations seldom follow true simple harmonic motion. A system that continues its motion indefinitely without losing its amplitude is termed undamped. However, friction of some sort usually dampens the motion, so it fades away or needs more force to continue. For example, a guitar string stops oscillating a few seconds after being plucked. Similarly, one must continually push a swing to keep a child swinging on a playground.
Although friction and other non-conservative...
Although friction and other non-conservative...
5.6K
Root Loci for Positive-Feedback Systems
88
The Hartley oscillator is a positive feedback system that sustains oscillations by feeding the output back to the input in phase, thereby reinforcing the signal. Positive feedback systems can be viewed as negative feedback systems with inverted feedback signals. In these systems, the root locus encompasses all points on the s-plane where the angle of the system transfer function equals 360 degrees.
The construction rules for the root locus in positive feedback systems are similar to those in...
The construction rules for the root locus in positive feedback systems are similar to those in...
88
Oscillations about an Equilibrium Position
5.3K
Stability is an important concept in oscillation. If an equilibrium point is stable, a slight disturbance of an object that is initially at the stable equilibrium point will cause the object to oscillate around that point. For an unstable equilibrium point, if the object is disturbed slightly, it will not return to the equilibrium point. There are three conditions for equilibrium points—stable, unstable, and half-stable. A half-stable equilibrium point is also unstable, but is named so...
5.3K
Standing Waves in a Cavity
850
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
850

