Nana, Direct Internal connection to God, WWG1WWA, MAGA, Angels are here already #FightLikeGodIsBesideYou
All you have to do is Google or Duckduckgo:
Frequency music sleep
Frequency music God
Frequency music 8 hour
Frequency music healing
Frequency music DNA
Frequency music Love
Pick your desired result.
Dont expect things to happen overnight sometimes it takes a while, the more grounding you do and the more you cleanse your body and pineal gland the more the return.
I also drink no more than 10 oz of tonic water with quinnine per day along with a vitamin regimine.
I heard today that apricot juice is a good cleanser too, gonna try that. No floride! Research cleansing pineal gland & groun
Frequency music and... Quantum Dots?
https://aip.scitation.org/doi/10.1063/1.5126670?af=R&feed=most-recent&
Eigenfrequencies or natural frequencies are certain discrete frequencies at which a system is prone to vibrate. Natural frequencies appear in many types of systems, for example, as standing waves in a musical instrument or in an electrical RLC circuit.
An RLC circuit is an electrical circuit consisting of a resistor, an inductor, and a capacitor, connected in series or in parallel. The name of the circuit is derived from the letters that are used to denote the constituent components of this circuit, where the sequence of the components may vary from RLC.
LCR series circuit is also known as tuned or acceptor circuit. They have many applications particularly for oscillating circuits. Series LCR circuit has applications in radio and communication engineering. They can be used to select a certain narrow range of frequencies from the total spectrum of ambient radiowaves.
A series RLC network (in order): a resistor, an inductor, and a capacitor
A single-electron transistor (SET) is a sensitive electronic device based on the Coulomb blockade effect. In this device the electrons flow through a tunnel junction between source/drain to a quantum dot (conductive island).
Schematic of a basic SET and its internal electrical components.
Here we investigate high frequency AC transport through narrow graphene nanoribbons with top-gate potentials that form a localized quantum dot. We show that as a consequence of the finite dwell time of an electron inside the quantum dot (QD), the QD behaves like a classical inductor at sufficiently high frequencies ω ≥ GHz.
When the geometric capacitance of the top-gate and the quantum capacitance of the nanoribbon are accounted for, the admittance of the device behaves like a classical serial RLC circuit with resonant frequencies ω ∼ 100-900 GHz and Q-factors greater than 10(6). These results indicate that graphene nanoribbons can serve as all-electronic ultra-high frequency oscillators and filters, thereby extending the reach of high frequency electronics into new domains.
This chapter discusses three subjects, the quantum capacitance, the size-dependent dielectric function, and the doping of a quantum dot. The main difference in quantum capacitance from its classical definition is the fact that there is no such thing as storage of charge alone and the charge of electron is discrete. The classical capacitance taking into account the discreteness of electronic charge is quite different when there are only few electrons.
Only when the number of electrons is large does the discreteness of electronic charge cease to exhibit new features. When the size is below a couple of nanometers, quantum mechanically the kinetic energy of the stored electrons becomes dominant over the electrostatic stored energy. Pauli's exclusion principle plays an additional role in quantum capacitance.
The size-dependent dielectric function is not defined according to the usual definition, because of the loss of the global nature. It has been emphasized that even the general É›(q) is global while É›(a), with its boundary condition, is closer to the definition of localized response function. Using a single oscillator placed at the Fermi energy of all the valence electrons without any other adjustable parameter, the calculated value for silicon turns out to be almost identical to É›(q = 2Ï€/a), obtained from pseudopotential calculation.
