|
|
| On the 11. International Conference "Biological
Cancer Defense" in Heidelberg (May 3-5, 2002) |
INTERNATIONAL INSTITUTE
OF BIOPHYSICS
Basic
theory of cancer development and defense
At the 11th International Conference on "Biological Cancer Defense"
in Heidelberg (May 3-5, 2002), Prof. Popp presented his basic theory on
cancer development and defense. This was successfully discussed not long
ago at the Cancer Research Institute in Heidelberg (DKFZ), too. In view
of the positive response of scientists and because of his totally controversal
ideas at rather clear evidence, we think it worthwhile to publish the main
substance of Popp`s theory in a short review:
Popp pointed out that the death rate of cancer disease did not drop over
the last years, but increased significantly (Fig. 1,
(1)) This indicates that main stream science follows a completely wrong
direction. Popp compared these wrong steps with the attemps to find a
scientific answer to the question: How high is the temperature of a gas?.
If one catches the gas molecules and investigates them under the microscope,
the technique may improve step by step to electron microscopy and even
higher resolution microscopy. It will, however, always fail to produce
any essential result concerning the temperature of the gas. This includes
even a result that would inform the investigator in case his trials go
into a entirely wrong direction. Tumor growth is certainly also nothing
else than a collective phenomenon of the cell population. Consequently,
the central questions should be focussed on the control of cell division
rate rather than on molecular properties of single cells. A basic example,
and at the same time the starting point, of Popp´s theory is the
cell division, i.e. the mitotic figures (Fig. 2a).
As it is well known, the molecular content is divided into two identical
parts where the daughter cells contain always just half of the whole biomolecules
without deviations, while the statistical laws require an overshoot or
undershoot of ,
where N is the number of molecules. This would be about 105 molecules
more or less in always one of the daughter cells. The fact that practically
no aberration takes place can be explained only in terms of a regulating
electromagnetic field that stabilizes itself by interaction with the cell(s).
The electric and magnetic forces take care about the correct movement
(and reactions) of all the molecules. Actually, such a field is known
and can be calculated. It is the electromagnetic field within conducting
and/or dielectric cavities which spreads out over the interior of a cell
according to the Maxwell equations. The field pattern (local field strengths)
follows the classical laws of the Maxwell equations, whereas the dynamics
is subjected to quantum optics. Fig.2b displays such
a spatial field pattern which has been calculated by taking account of
the boundary conditions of a cell. (2). Those electromagnetic quasi-stationary
electromagnetic field patterns spread over the wavelength range from at
least about 200 to 800 nm (2). Table 1 displays the
series of cavity resonator modes in the optical frequency range. Their
superpositions fully explain the mitotic figures for stationary patterns
as well as in the course of time for the temporal sequence of superpositions.
The electric charges and magnetic moments of the molecules strictly follow
the electric and magnetic field pattern of the corresponding cavitity
resonator waves, respectively. As a consequence, the perfect spatio-temporal
distribution of molecules can be understood, and it is not wrong to say
that it can be understood only in this way. At the same time one has to
expect that an ideal photomultiplier should register photons outside of
the cell population just within this wavelength range of, say, 200 to
800 nm (3). In addition, since these field patterns represent coherent
states, the probability of measuring n photons has to follow Poissonian
photocount statistics p(n) = exp (-<n>) <n>n/n!. Both is true
(3,4) The evidence of these "biophotons" (which are emitted
as single photons by living biological cells and systems satisfying just
these conditions) has been shown by Popp´s group since 1976, and
has been reproduced by several other scientists working on the field of
biophotonics. We will not repeat the confirmation of all these results,
but like to refer to our bibliography (www.lifescientists.de/publication/bibliography1-1.htm
or www.biophotonik.de).
Popp confined in Heidelberg to the aspects concerning cancer development.
Since a coherent field is self-reflective, it follows laws like
¶ /¶
t (n) = a n + b n2 (equ.1),
where n are subunits of the system (i.e. photons or cells), ¶
/¶ t (n) describes the time development
of n, and a and b are parameters. b must not vanish in order to keep the
coherence of the system. A typical example is the correlation between
biophoton emission and cell growth (Fig. 3), where
b<0 provides the saturation of cell mass and inhibits overshoot of
cell growth, while a>0 is necessary for cell growth stimulation. While
a may refer to chaotic components, b is a collective parameter, dependend
on intergrative properties of the whole cellular system. b as inhibitor
of cell growth is strongly linked to the degree of the coherence of the
field. Consequently, a definite loss of coherence is a necessary and sufficient
condition of cancer development (5,6). The cancer problem is reduced to
the investigation of b and b/a.
Actually, Schamhart et. al. and Scholz et.al.showed that the loss of the
validity of equ.1 and the loss of coherence, which can be expressed in
terms of b and a, is strongly correlated to the cancer growth (Fig.
4 and Fig.5, (7,8)). This correlation has the
power of a causal relation, since it does not only lead to quantitative,
but also to qualitative differences between "normal" cells and
"tumor cells" without any exception.
As soon as we arrive at this stage, there is already a powerful strategy
and tool for overcoming the malignancy of cancer development. In case
the tumor tissue is available (surface tumors or tissue after operation),
one may expose the tumor tissue to non-toxic agents and examine whether
the biophoton emission will increase or decrease under this treatment.
For the case of increase (which happens in most cases) the remedy or therapeutic
trial under examinations is helpless. However, if the application of the
remedy (agent) leads to a decrease of the biophoton emission, one may
provide that the application results in an improvement of the state and
may even heal the disease. Our experience shows that in such a case the
normal cells, always being present in a real tumor, are likely to be activated
to remove or suppress the tumor cells. This therapy follows just the opposite
strategy from the usual tumor therapy. Instead of killing tumor cells
(and the connected normal tissue), it stimulates the normal tissue for
overcoming malignancy of the whole cell population, in other words to
provide b<0 of equ.1. This may be a physical influence, simply improving
the transparency of the tissue under examination. Obviously, the suitable
remedy that has to be individually adapted to every case improves the
degree of coherence within the tissue under investigation. This may happen
also in the well-known cases of "spontaneous remission" of cancer.
This therapy has the disadvantage that an operation might be necessary
in order to find the suitable remedy. However, Zhang and Popp (9) have
shown that the loss of coherence can get measured to some degree not only
by investigating the biophoton emission of the tissue or of the body (10),
but also by statistical analysis of physiological parameters, i.e. resistance
(or conductivity) values of the body. Coherence of regulating fields is
strongly related to the log-normal distribution of physiological parameters,
a fact that is well known in statistical medicine under the name of "multiplicative
Gestaltungs-principle". As soon as the coherence gets lost, the log-normal
distribution of conductivity values of the skin more and more turns into
a Gaussian distribution. Fig. 6 shows an example.
A German company developed an electrode that enables us to measure hundreds
of conductivity values of the human skin in a rather short time. After
suitable adjustment of the measurement values the statistical distribution
is available and provides a rather reliable indicator of the degree of
coherence of the field within the human body. In a non-invasive way one
may follow then rather comfortably the state of disease and its development
under treatment.
Just in view of new confirmation (11-13), it seems useful to follow this
theoretical concept and the idea of measuring the degree of coherence
of the biophoton field in a living system in order to open the door in
understanding and overcoming cancer.
References:
(1) Welt am Sonntag Nr. 15, 14.04.2002, p. 37: Wissen Medizin, Krebszellen
in Schach halten.
(2) F.A.Popp: In: Electromagnetic Bio-Information (F.A.Popp, G.Becker,
H.L.König, and W.Peschka, eds.), Urban & Schwarzenberg, München
1979, pp. 123-149.
(3) F.A.Popp, B.Ruth, W.Bahr, J.Böhm, P.Grass, G.Grolig, M.Rattemeyer,
H.G.Schmidt, and P.Wulle: Collect.Phenom.3 (1981), 187.
(4) J.J.Chang, J.Fisch, and F.A,Popp: Biophotons. Kluwer Academic Publishers,
Dordrecht-Boston 1998.
(5) F.A.Popp: In: Recent Advances in Biophoton Research and ist Applications
(F.A. Popp, K.H.Li and Q.Gu, eds.): World Scientific, Singapore-London
19992.
(6) F.A. Popp: In: Macroscopic Quantum Coherence (E.Sassaroli, Y.Srivastava,
J.Swain, and A. Widom, eds.), World Scientific, Singapore-New Jersey,
pp. 130-150.
(7) D.H.J.Schamhart and R.van Wijk: In: Photon Emission from Biological
Systems (B.Jezowska-Trzebiatowska, B.Kochel, J.Slawinski, and W. Strek,
eds.), World Scientific, Singapore (1987), pp. 137-152.
(8) W.Scholz, U.Staszkiewicz, F.A.Popp, and W.Nagl: Cell Biophysics 13
(1988), 55-63.
(9) C.-L. Zhang and F.A.Popp: Medical Hypotheses 43 (1994), 11-16.
(10) S.Cohen and F.A.Popp: J.Photochem.Photobiol.B: Biol.40 (1997), 187-189.
(11) New Scientists Archive, Feb. 22, 2002: Body talk.
(12) F.A.Popp and Y.Yan: Phys.Lett.A 293 (2002), 93-97.
(13) F.A.Popp, J.J.Chang, A.Herzog, Z.Yan and Y.Yan: Phys. Lett. A 293
(2002), 98-102.

Fig. 1: There is a strong increase of tumor death rate since 1990
in US. 

(a) |

(b) |
Fig.2a: An example of a mitotic figure of a cell in a definite stage.
Fig.2b: The Electric Field of a TM (1,1) cavity mode provides the field
strength that is necessary to establish the mitotic figure of Fig.2a.
|
TE mode
mnp
|
TM mode
mnp
|
wavelength
l /nm
|
|
111
|
|
690
|
| |
010
|
574
|
|
112
|
|
571
|
| |
011
|
546
|
| |
012
|
481
|
|
113
|
|
462
|
|
211
|
|
438
|
| |
013
|
410
|
|
212
|
|
402
|
|
114
|
|
379
|
| |
110
|
360
|
|
213
|
|
358
|
|
011
|
111
|
353
|
| |
014
|
349
|
|
012
|
112
|
333.5
|
|
311
|
|
323
|
|
115
|
|
318
|
Table 1: Cavity Resonator Modes which are stabilized in cells. They are
necessary and sufficient for displaying the spatio-temporal dynamics of
mitotic figures.

Fig.3: Emission of biophotons during the growth of seedlings (left)
and growth itself (right). There is a strong correlation between cell
division rate and biophoton intensity according to¶
/¶ t (n) = an + bn2,
where a>0 and b<0. 

Fig.4: While the biophoton emission drops down for normal cell populations
with increasing cell density (lower curve), it increases for cancer cells
(upper curve). b turns from a value <0 to one which is >0, as soon
as normal cells change to cancer cells (see reference (7)). 

Fig.5 While normal tissue increases the degree of coherence of the
biophoton field with increasing cell density, tumor tissue decreases the
degree of coherence of the biophoton field (see reference (8)). The lower
curve represents normal cells, the upper curve tumor cells. The ordinate
displays a measured value, representing the deviation from ideal coherence,
the abscissa the number of cells in the measuring cuvette. 
(a)
(b)
Fig. 6: The distribution of the frequency of measuring definite values
of skin conductivity of a healthy person (Fig 6a) and of a cancer patient
(Fig.6b). While the distribution of a healthy person follows a log-normal
distribution, the one of a cancer patient turns into a Gaussian distribution,
reflecting the coherence and the chaotic state of the biophoton field,
respectively.
Remark on equ.1).
Popp and Chang (F.A.Popp and J.J.Chang. Sci.China C 43(2000), 507) showed
that by phase conjugation effect zones of destructive interference in
the intercellular space and, on the other hand, zones of constructive
interference in the intracellular space may be responsible for communication
and organization effects in and between living organisms, including cell
tissues. This means that from the energetical point of view the growth
regulation origins from a balance equation (equ.2):
N (grad E) D x = E (equ.2),
where N is the number of cells, E the whole free electromagnetic energy
and D x the thickness of the double layers
between the zones of destructive and constructive interference. Grad E
is ¶ E/¶
x over these zones which is responsible for the attractive force between
cells.
Let us define now average values over a considerably long time interval
of some minutes:
- -1/N<¶ /¶
t (grad E)/grad E> = b, where b< 0 according to the paper by Popp
and Chang, since the force is attractive for increasing gradient.
- - <¶ /¶
t(D x)/D
x> = a, where a>0 according to this paper since the force increases
with decreasing thickness of the double layer.
Then a straight-forward calculation of ¶
/¶ t (N (gradE) D
x) = (¶ /¶
t E) = 0 leads to the growth equation:
¶ /¶
t N = aN + bN2
This equation shows that from the energetical point of view cancer develops
for b³ 0 which means that the energy is
not transportable into the cancer tissue. Cancer is then a problem of
energy distribution, transparency and coherence rather than of a causal
energy deficiency. At the same time one has to consider that by the lack
of coherent electromagnetic energy the repair and communication system
between cells gets damaged.
International Institute of Biophysics | Research Groups | News/Recent Publications
© International
Institute of Biophysics 2002 E-mail: iib@lifescientists.de
|