scholarly journals Entelechy, Gyroscopes, and QBism: developing a Quantum Metaphor for the vital force

Author(s):  
Lionel Milgrom

Background Entelechy (e.g., Hahnemann’s Vital Force, Vf), bears striking similarities to certain properties of quantum systems. Thus, the Vf is only indirectly observable via (centrifugally) expressed symptoms: a quantum property is only indirectly observable via its experimental effects. Consequently, a quantised Vf ‘gyroscopic’ metaphor is proposed where ‘axial’ rotation (represented by a wavefunction) undergoes dis-ease-induced retardation leading to Vf ‘precession’, i.e., symptom expression. Remedy-induced acceleration of axial rotation results in cure, via centrifugal removal of dis-ease, so precession/symptom expression ceases. The Vf ‘gyroscope’ is considered quantised partly because patients are observed during ‘discreet’ appointments, not continuously. Objective To develop this metaphor further by generating wavefunctions to represent the Vf in various states of dis-ease and health. Method Three wavefunctions are generated from secondary symptoms exhibited by the patient’s Vf, as observed by the practitioner. Three more wave functions are generated from analogous (unobserved) hypothetical states, representing the Vf evolving from health into a precursor dis-eased state. Results and discussion The evolution of therapeutic/dis-ease processes are imagined as transformations between these Vf wavefunctions, visualised as patient states on six of the nine points of an enneagram. The remaining three points represent practitioner states, ‘entangled’ with these processes. The Vf states may be divided into two groups - one indirectly observable via expressed symptoms, the other hypothetical - separated by a notional therapeutic ‘event horizon’. The practitioner, Janus-like, manages the therapeutic process by ‘negotiating’ between these two groups. Conclusion An interpretation of quantum theory called QBism (i.e., Quantum Bayesianism, in which a wavefunction represents only the total subjective information available to an assigning agent, not a shared separate objective reality), suggests these various Vf wavefunctions could represent Chalmers-like non-reductive information states, proposed as starting points for considering the influence of consciousness on the therapeutic process.

2019 ◽  
Vol 27 (1) ◽  
pp. 6-18 ◽  
Author(s):  
Lionel R. Milgrom

Background: Many complementary and alternative medicine modalities consider the vital force (Vf) an organism’s source of health and healing, Hahnemann’s notion of the Vf having similarities with quantum systems. Thus, the Vf is only indirectly observable via expressed symptoms: a quantum property is only indirectly observable via its observed experimental effects. Objective: To develop further a quantised gyroscopic metaphor of the Vf in which dis-ease slows axial rotation, causing the Vf to precess (i.e., express symptoms). The curative remedy accelerates axial rotation, throwing off the dis-ease, so precession (and symptom expression) cease. Method: Using earlier wave functions depending solely on observed patient symptoms and changes to them, 6 further wave functions are generated, representing the Vf in various states of dis-ease and health. Results: All 6 Vf wave functions can be arranged on 6 of the 9 points of an enneagram, the other 3 representing the practitioner. Conclusion: Transformations between the 6 Vf states are readily visualised. They may also be divided into two groups separated by a therapeutic “event horizon,” the practitioner being the “arbiter” between them. Thus, they could represent non-reductive information states, suitable as starting points for understanding the influence of consciousness on the therapeutic process.


1988 ◽  
Vol 31 (2) ◽  
pp. 169-189 ◽  
Author(s):  
E.B. Bogomolny

Author(s):  
Kevin Kögler ◽  
Phan Thành Nam

AbstractWe consider an analogue of the Lieb–Thirring inequality for quantum systems with homogeneous repulsive interaction potentials, but without the antisymmetry assumption on the wave functions. We show that in the strong-coupling limit, the Lieb–Thirring constant converges to the optimal constant of the one-body Gagliardo–Nirenberg interpolation inequality without interaction.


Author(s):  
I.Z. Tsekhmistro

In modern physics the common relational approach should be extended to the concepts of element and set. The relationalization of the concepts of element and set means that in the final analysis the World exists as an indivisible whole, not as a set (of one or another kind of elements). Therefore, we have to describe quantum systems in terms of potentialities and probabilities: since quantum systems cannot be analyzed completely into sets of elements, we can speak only of the potentialities of isolating elements and sets within their structure. On the other hand this quantum property of the world as an indivisible whole accounts for the astonishing logical properties of the structure of the potentialities of quantum systems which it brings forth. This has been confirmed by quantum-correlation experiments (A.Aspect and oth.). These effects have a relational nature, not a physical-causal or material one, and they are brought forth by the changes (resulting from measurement or physical interaction) in the structure of the relations of the mutually complementary sides of reality. One of these sides expresses an actually existing structure of the system as a real (and physically verifiable) but only relatively separable set, and the other expresses the sets of potentialities in it which arise from the astonishing property of finite non-analyzability of the system into elements and sets (i.e. by the quantum property of the world as an indivisible unit).


1997 ◽  
Vol 78 (17) ◽  
pp. 3229-3232 ◽  
Author(s):  
T. Hatsuda ◽  
T. Kunihiro ◽  
T. Tanaka

2011 ◽  
Vol 26 (05) ◽  
pp. 351-358 ◽  
Author(s):  
GUO-HUA SUN ◽  
SHI-HAI DONG

New type shift operators for three-dimensional infinite well potential are identified to connect those quantum systems with different radials R but with the same energy spectrum. It should be pointed out that these shift operators depend on all variables contained in wave functions. Thus they establish a novel relation between wave functions ψlm(r) and ψ(l±1)(m±1)(r).


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