Advanced Space Weapons Physics Principles Lecture 1

Technique I (not the only way perhaps)

On Jan 4, 2006, at 6:34 PM, d14947 wrote:

Jack you (inadvertently:] point to an important issue.

It was advertent.

....
After all, if we already have precognition, PK and so on, we may also be able to operate the fields (Higgs electroweak?) that would allow us to have a warp drive, right? Then we could join the big kids in the galactic playground.

Lenny Susskind says one cannot manipulate the electroweak Higgs field over large volumes - it is too stiff at 10^40 Joules per cc. He is correct. However he means the Higgs intensity. I manipulate the Goldstone Phase. Of course, the two may be connected nonlinearly. However, there is more than one Higgs field. The electroweak Higgs field give the masses of the elementary leptons & quarks, but it's the Planck Scale Higgs field's 2 Goldstone phases that gives gravity.

In the simple case of n = 2 with only one Goldstone phase, toy model for simplicity.

Higgs Field = |Higgs Field|e^i(Goldstone Vacuum Phase)

For metric engineering we have

Higgs Field + Control Field

The important cross term is

2|Higgs Field||Control Field|cos[(Goldstone Vacuum Phase - Control Phase)

where |Higgs Field| STAYS CONSTANT as Lenny says.

&/\zpf ~ 2|Higgs Field||Control Field|cos[(Goldstone Vacuum Phase - Control Phase)

Goldstone Vacuum Phase - Control Phase = MODULATED VACUUM PHASE = Chi

BECAUSE the equilibrium Higgs field (/\zpf ) is very small, i.e. dark energy density ~ 0.73 critical density for flat space universe

(0.73)(8piG/c^4)(Critical Energy Density) = (/\zpf) = (Quantum of Area Flux)^-1[|Higgs Field|^2 - 1]

Where Higgs Field is normalized to a pure number.

(/\zpf) + &/\zpf = (Quantum of Area Flux)^-1[|Higgs Field + Control Field|^2 - 1]

&/\zpf = (Quantum of Area Flux)^-1[2|Higgs Field||Control Field|cos(Chi) + |Control Field|^2 ]

where Higgs Field||Control Field| >> |Control Field|^2

i.e. |Control Field|/|Higgs Field| << 1

TINY CONTROL SIGNAL is AMPLIFIED!


On Jan 4, 2006, at 4:12 PM, Jack Sarfatti wrote:


On Jan 4, 2006, at 3:30 PM, rkiehn2352@aol.com wrote:



-----Original Message-----
From: Jack Sarfatti
To: ROBERT BECKER
Sent: Mon, 2 Jan 2006 20:15:17 -0800
Subject: Hal Puthoff's "Matrix" paper examined

JACK
BE CAREFUL
The curvature tetrad field as an invariant Cartan 1-form is

RMK SAYS:
in my experience
USUALLY TETRADS ARE MATRICES OF FUNCTIONS, (0-FORMS),

By tetrad as used in GR is meant eu^a

guv = eu^anabev^b

ds^2 = guvdx^udx^v

The 4 tetrad 1-forms are then

e^a = eu^adx^u

So you probably call these e^a "co-frames"?


CO-FRAMES ARE MATRICES OF 1-FORMS,
CURVATURES ARE MATRICES OF 2-FORMS,
TORSIONS ARE VECTOR ARRAYS OF 2-FORMS.
CURRENTS ARE VECTOR ARRAYS OF 3-FORMS.


The integral of dA over closed surfaces surrounding point defects in the Higgs field is quantized as integers x (Planck Area).

THE HIGGS FIELD ACCORDING T0 ATIYAH AND MASON AND WOODHOUSE
IS AN EXACT DIFFERENTIAL, AND THEREFORE IT IS HARD FOR ME
TO ASSOCIATED THE HIGGS WITH A CLOSED 2-FORM.

I never said that dA is the Higgs field.

In my model, there are 3 real Higgs fields with 2 independent Goldstone phases theta & phi

I define

B/Lp ~ (dtheta)(phi) - (theta)(dphi)

Therefore

dA/Lp^2 = dB/Lp = 2(dtheta)/\(dphi)


Note that d^2A = 0 but we define a NONLOCAL Bohm-Aharonov "flux without flux" as

BOHM AHARONOV IS due to a non exact but
CLOSED 1-FORM, NOT A 2-FORM

I know. That would be like "Area without area." I have generalized the idea up one step to a nonexact closed 2-form.

In geometrodynamics, the generalized B-A effect gives the quantized world hologram of "Volume without volume".

That is B is a geometrodynamics "line form".

dB is a geometrodynamics "area form"

d^2B = 0 would be the volume form, but it is locally zero. So I get QUANTIZED nonlocal "volume without volume"

i.e. integral of the geometrodynamic AREA FORM dA over closed non-bounding surface surrounding a point defect in the Higgs vacuum order parameter is Lp^2 Integer.

It is AS IF there were a volume 3-form d^2B - it's locally zero but nonlocally not zero - it's the ghostly volume integral of "zero" d^2B that I DEFINE as equal to the surface integral of dB in a "singular" extension of the Gauss theorem.

This is VOLUME WITHOUT VOLUME = World Hologram

Let d = exterior derivative on p-forms p -> p +1

& = boundary operator on p-coforms p -> p -1

Then in obvious Dirac notation where the "bra-ket" is a DeRham integral

(p|&p+)> = (dp|p+1)

OK I DEFINE

|&'p+1) to be a closed p coform that is not a boundary of a p+1 coform.

That is &|&'p+1) = 0

A stargate portal has this property where p = 2 because the p + 1 space is multiply connected with "wormholes".

BY DEFINITION

(p|&'p+1) = (d'p|p+1) ~ Integer

When the p-homotopy group is non-trivial

(dp| is locally zero

but

(d'p| is a GHOSTLY nonlocal "flux without flux" p+1 form that does not vanish in the DeRham integral sense.

This also explains why gravity energy is nonlocal and why the Yilmaz theory is wrong.

In ordinary vacuum the total gravity energy density is locally zero, but that does not prevent a non-zero Poynting flux of gravity wave energy flow through a closed non bounding surface surrounding the source of the gravity waves.