The possibility of Topological Materials on the Lunar Surface.

Caption to the Photo: KVNarasinga Rao carried out the experimental research at the Dept.of Electrical Engrg., University of Illinois, Urbana, Illinois, USA during the years 1954-1961.

The possibility of Topological Materials on the Lunar Surface.
By Professor Kotcherlakota Lakshmi Narayana,

Key words: Plasma Diagnostics, Microwaves, Rao particles, Magneto tail,
Conventional Spectroscopy, Sensing Signal Technique, Collision Frequencies,
Lunar Dust, Chandhrayana Mission.
14th May 2008 : Time 8:00PM.IST
http://trusciencetrutechnology.blogspot.com/

The surface of MOON is constituted by Lunar Dust, loose material, rocky and Boulder formations, and it has several secrets that it holds at its bosom.[1,2] The contention of present author, is that the material of the Moon, gets topologically excited, under disturbed conditions. The Plasma Sheet, the Earth’s magneto tail, [3], solar stream wind/particles, Cosmic and Asteroid debris etc produce those disturbed environments.
The Lunar probes, like the Chandhrayana Mission need to be planned to incorporate devices that might possibly reveal the material properties of the Moon. The topological excitation of the Molecular/Crystalline force fields has been extensively reported, by the present author, in a series of articles [4].
The Topological Excitation acquiring a Charge and as well a Spin, has been termed as Rao particle. The Rosfet Device [5] is a spin-off of a research study on these excitations.
The Electron gets “entangled’ with the Rao particles [6], which the later are of two types, a Rao particle and the other an Anti-Rao (AR) particle. AR-Electron forms a pair, like the Electron-Hole (the exciton). But the Rao and Anti-Rao are topological particles that posses a winding number.
The richness of concept of topological excitations, generated in the material on the surface of Moon in disturbed environments, is quite vivid.
The Electrons of the Molecular/Crystalline-like structures of the Lunar surface Material, gets involved with the Rao and Anti-Rao particles. The floating [7] electrically charged dust (observed by NASA’s Lunar Prospector and NASA’s Surveyor 7 Lander) as reported by Space.com staff [8] also gets associated with topological excitations to form the New Bosons.
This physical feature provides immense possibilities of exciting research on Lunar Dust. The finding that Electrons pepper the Moon Surface has therefore an explanation in the present formulation and Model considerations by the present author.
Thus the Moon’s surface Material with the Mentioned topological excitations, offers a comfortable bed, for the resting Electrons. In two ways, it can happen. How they differ? Firstly, the free electrons/or the lone pair Electrons Spin and Charge may be absorbed in the bed of topological excitations. Next path way is that such Charged and Spinning, topological excitations, get associated with the peppering Electrons, to form a New Gas of Bosons.
Use of Rosfet Device to investigate the Characteristics of these topological excitations is one technique.
But more profound is the applicability of the Generalized [9] Dr.K.V.N.Rao’s SST (sensing signal technique) at different Electromagnetic frequencies. This technique is more powerful than the conventional Spectroscopy methods of analysis. [10] (See the photo and the Caption given)
Caption to the Photo: KVNarasinga Rao carried out the experimental research at the Dept.of Electrical Engrg., University of Illinois, Urbana, Illinois, USA during the years 1954-1961.

Dr.K.V.N.Rao’s generalized SST helps to launch more than one sensing signal to understand the disturbed Plasma Environment, of the Lunar surface and its embedded atmosphere. Compact Space Probes based on Dr.K.V.N.Rao’s SST would be a boon to Lunar/Chandhrayana Missions being planned in a global enterprise.
Either of the mentioned Devices, help to understand the AIRGLOW, [11], Gaseous Discharges and Microwave Plasma Diagnostics [12] of the Moon.
Reverting to a discussion on the Rao particles, proposed by the present author, it is to be noted such a particle, has. a characteristic winding number. This feature is the strength of the new formulation proposed. The winding number decides the effective mass possessed by the Rao particles and the Binding Energy levels of the “AR-Electron” Boson.
With the temperature, on the Lunar surface, ranging over far below freezing and to high temperatures beyond 1500 degree Kelvin it offers, transition features, of certain properties, of the Lunar Material.
The interactions responsible, for the transitions, have coupling constants that generate Direct or Exchange contributions to the Energy levels of the New Boson.
The material on the Moon has definitely certain internal fields. Obviously, the topological excitations of the material on the surface of Moon is a subject

References:
1. Thursday, February 21, 2008

The Fourth Week of February 2008 Lunar Eclipse with Romantic Blue http://trusciencetrutechnolgy.blogspot.com
2. Space.com staff “Strange Things Happen at Full Moon” posted 18th April 2008 at 01:51pm ET
3. Tim Stubbs, University of Maryland, Goddard Space Flight Centre.
4. a) “The Spin Polarization of Molecular vibrations and Peram Manifold of XY4 type metallic Complexes (Molecules) (KLN) 69th session of .Ind. Sci Cong.Chem Sect, p.171, IV 6-1-1982, Mysore University, India.
b).”Spinorial Optics of Structural Vibration of Ions and the Quasiparticle Quantization of Rangadhama Effect “(KLN) 70th Proc. Ind.Sci.Cong.Part III, Tirupati, Sri Venketeswara University, 6-1-1983.
c). ‘Renormalization of Vibrational energy by Rangadhama Quanta and Spinorial phase transitions” (KLN) 71st sess. Ind Sci.Cong.Paper.216, p.102, Chem IV, Ranchi, 1984.
5. “Rosfet device the Electronic Liquid Characteristics, Model and Theory of Rosfet Device” Paper No.112, p.69 Sect.XIII Physical Sciences., Proc. 94th ISC,
Jan 3 -7, 2007, Annamalainagar, Chidambaram.
6. Rao particle termed in memory of Late Prof. K.Rangadhama Rao D.Sc (Madras) D.Sc. (London)
7. NASA’s LUNAR PROSPECTOR and NASA’s Surveyor 7, Lander photo of a Strange Glow. (See reference no.11 below)
8. Space.com staff “Strange Things Happen at Full Moon” posted 18th April 2008 at 01:51pm ET
9. K.V.Narasinga Rao et al.” Interaction of Microwaves in Gaseous Plasmas Immersed in Magnetic fields” Proceeding of IRE, p.1877-1889,Vol.49.No.12, December 1961.In this article it is asserted that “Even modest amplitudes of resonating wave, the kinetic energy of the electrons increases considerably, which in turn effects (10 The electron collision frequency and (2) The magnetic field control of the plasma confinement”
10. KVNarasinga Rao carried out the experimental research at the Dept.of Electrical Engrg., University of Illinois, Urbana, Illinois, USA during the years 1954-1961.
11. Observation of the peculiar zingling glows over the onset of eclipse of Moon was first reported on 4th April 1996 by Dr.K.L.Narayana. They were observed by a telescope behind his staff quarters in Shivaji University,Kolhapur-416004,India,during 12.15 to 12.30AM on the 4th April The eclipse was observed as %(time) sequence 10%(3.59) ,20%(4.09),50%(4.25),70%(4.60) and 100%(4.59) in the morning time (see report in SAKAL News Paper, Kolhapur, Maharashtra State, edition dated 5th April 1996.)
12. Book “Plasma Diagnostics with Microwaves” ,John Wiley & Sons Inc,NY(1965), by M.A.Heald and C.B. Wharton, Page 92. { Ref: Rao et al: On experimental techniques to measure velocity dependence of Collision frequencies”}