The diagram illustrates the process of using laser beams with orbital angular momentum (OAM) to study the photoionization of a gas jet and the resulting photoelectron momentum distribution. The core components and their roles in the experiment are as follows:
•Input OAM beam (circularly polarized): This is an intense, twisted laser pulse that carries OAM and is used to ionize the atoms in the gas jet. Its spiral phase front is a key characteristic.
•Gas jet: This is the target material, typically an inert gas like argon, which is ionized by the OAM beam.
•Probing diffracted beam (circularly co-polarized): A second, weaker laser beam is used to probe the interaction and alter the momentum of the ionized electrons, which helps to distinguish between different OAM states.
•Photoelectron momentum distribution: The ionized electrons (e-) are ejected and their momentum distribution is measured. This distribution, which appears as a ring or a more complex pattern, provides information about the interaction of the OAM beam with the atoms.
•Output OAM beam (unaffected): The primary OAM beam continues on its path after interacting with the gas jet. The method is considered "nondestructive" to the original pulse, meaning the pulse itself is not significantly altered.
The experiment is a theoretical and computational approach to study strong-field ionization. It aims to develop a method for determining the magnitude of the OAM carried by a laser beam by analyzing the momentum of the photoelectrons.
Intense laser ionization expands Einstein's photoelectric effect rules giving a wealth of phenomena widely studied over the last decades. In all cases, so far, photons were assumed to carry one unit of angular momentum. However it is now clear that photons can possess extra angular momentum, the orbital angular momentum (OAM), related to their spatial profile. We show a complete description of photoionization by OAM photons, including new selection rules involving more than one unit of angular momentum. We explore theoretically the interaction of a single electron atom located at the center of an intense ultraviolet beam bearing OAM, envisaging new scenarios for quantum optics.
The image is a schematic diagram of a multibeam rotatable terahertz (THz) array antenna.
•The antenna is based on metallic waveguides.
•It shows how two orthogonal polarization components, 
•E
T
E
𝐸
𝑇
𝐸
and 
•E
T
M
𝐸
𝑇
𝑀
, are combined to produce a rotating beam.
•The control unit is a metallic waveguide with dimensions 
•a
𝑎
,
•b
𝑏
,
•h
ℎ
, and wall thickness 
•T
𝑇
.
•The three-dimensional radiation patterns of the antenna are shown under different phase differences between the two orthogonal polarization components.
To the point
This is key
The one
Positive +
A separation of charge dipole moment
Relax
Electron hole or proton recombination emitting light
Free energy in theory
Kee P+ in G on
Rotate the dipole
Two separation of vortices within a vortex
God bless
Optical metasurfaces for generating and manipulating optical vortex beams
Take a guess here.
Lipid optical metasurfaces are specialized nanostructured surfaces that combine the unique optical properties of metasurfaces with the biochemical characteristics of lipid membranes. This platform is used to create highly sensitive, label-free biosensors for advanced biological and medical applications. By coating a metasurface with a biomimetic lipid layer, researchers can study dynamic molecular interactions in real-time with exceptional sensitivity.
•AI and deep learning algorithms can be applied to analyze the rich spectral data obtained from metasurface biosensors. This helps extract features and classify complex molecular behaviors, such as the photoswitching dynamics of lipid membranes.
•Tunable platforms: While some metasurfaces are static, active materials like liquid crystals or graphene can be integrated to create reconfigurable metasurfaces. This allows for dynamic electrical control over the optical properties for applications like sensing and dynamic displays.
One more time
ON OFF…
OFF… ?
TURNING OFF TWO WAVES OF THE SAME FREQUENCY AS A CIRCULAR STANDING WAVE RESONATING WITHIN
🫶🏻
• • •
Missing some Tweet in this thread? You can try to
force a refresh
Keir Starmer is playing Russian roulette with our lives.
•Neuromodulation: It can be used for highly precise optogenetic neuromodulation.
•In Vivo Optogenetics: The technique has been demonstrated to evoke more significant motor behavior and neuronal activation in vivo.
•Synthetic Biology: It has potential applications in synthetic biology, contributing to the development of advanced tools for controlling cellular activity
This diagram illustrates the phenomenon of total internal reflection, where a standing wave is formed in a dense medium and an evanescent wave is created in a rarer medium.
•Standing Wave: This wave is formed in the denser medium (
•n
1
𝑛
1
) due to the interference between the incident and reflected waves. The wave oscillates in time, but its peak amplitude profile remains stationary in space. The wavelength of the standing wave is denoted by 
•λ
e
x
𝜆
𝑒
𝑥
.
•Evanescent Wave: This is a non-propagating electromagnetic field that exists in the rarer medium (
•n
2
𝑛
2
) near the interface. Its amplitude, 
•E
𝐸
, decreases exponentially with distance (
•z
𝑧
) from the interface. The characteristic distance over which the amplitude falls to 
•1
/
e
1
/
𝑒
of its value at the interface (
•E
0
𝐸
0
) is called the penetration depth, denoted by 
•d
p
𝑑
𝑝
. The evanescent wave does not carry energy away from the interface but its presence is crucial for the reflection process.
The inner circle
Quantum tunneling occurs when a wave, acting as a potential barrier, forms an evanescent field that decays exponentially but still allows a portion of the wave to penetrate and emerge on the other side with reduced amplitude, a phenomenon that applies to both quantum particles and classical waves like light
•Neutral atoms: have an equal number of protons and electrons, making them electrically neutral.
•To become a cation, an atom must lose one or more electrons, typically from its outermost shell.
•The loss of these negatively charged electrons leaves the atom with an imbalance of charges, where the number of positive protons is greater than the number of negative electrons.
•This imbalance creates a net positive charge on the ion, which is then called a cation
@Martha_Sheshan @Allibab97431613 @loganrunagain @Shannon21599100 @MikeM2014 @BJamaste @missj75 @realSaltySeaDog @chargeadem @thundertanking @HannqverF @TanngrisnirGoat @treeninja390 @many_oneof @realsnozilla @falsely_flagged @pocketonashirt @SusanGrant60501 @TheDonallegedly @OlgaStaysTuned @BelonTuthk @RealCraigSawyer @bnd2024 @Ghostrider768 @vrotocol @JOSHGOLF77 @DontCallMeDuke @hillbe12 @BLarge @HeartSynthesis @realDevian @JeepAJoJo @ultragish52 @truestormyjoe @Gypsysoulwildh1 @PatriotPraetori @Rofiko00Aulia @cons @pSadButTrueq @Amy445393681 @realDonaldTrump @POTUS @Shorty56167141 @Fred_cpo @kurtcaz1 @DJEMEDIA_ The number of electrons lost determines the magnitude of the positive charge
Electrons are created primarily through the process of pair production, where a high-energy photon, like a gamma ray, converts into an electron and its antiparticle, a positron, in the presence of an atomic nucleus. This requires a minimum energy of 1.022 MeV and follows Einstein's E=mc² equation. Electrons are also created in the universe during beta decay of radioactive isotopes and in high-energy events like cosmic ray collisions.
Pair Production
•Energy into Matter: This is a quantum phenomenon where energy in the form of a photon transforms into matter and antimatter.
•Minimum Energy: The photon must have a minimum energy of 1.022 MeV to create an electron-positron pair, which is the combined rest mass energy of the two particles.
For a particle with a refractive index lower than the surrounding medium, a blue-detuned laser—with a frequency higher than the medium's resonance—causes the gradient force to be dominant. The net effect is that the particle is repelled from the center of the laser beam and pushed towards the areas of lower intensity. This is the opposite of a standard optical trap, or "optical tweezers," which uses a red-detuned laser to pull particles with a higher refractive index towards the focus