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P291. The law of the state of material communication




P291. The law of the state of material communication

The simultaneous states of any interacting material objects are necessarily the state of their connection. (3. 2. 2. ) 291

Any material connection, according to the law of material connection (200), is itself a material object, which in any of its states is completely determined by its many physical parameters (state matrix). At the same time, there are objectively matrices of states of the subjects of this connection.

 

P292. The principle of the matrix of the state of a material object

 The matrix of the state of any material object is a set of all its (state) physical parameters. Moreover, all these parameters must correspond to each other on the basis of belonging to one state of a material object. (3. 2. 2. ) 292

                                                         

This is a short addition to the previously formulated principle of the matrix of the state of a material object (236). This means that at the moment of reflection from a material source of information, all the parameters of the reflected quantum of light and all the parameters of this material source must belong to one state of their material connection, and therefore, to one matrix of this state. Thus, they necessarily correspond to each other.

 

P293. The principle of material conformity

Any state of any material connection is necessarily a mechanism for matching all the parameters of its objects, since all the parameters of its objects must necessarily belong to one matrix of the state of this connection. (3. 2. 2. ) 293

              

Any material connection is always a material object. And for her the law of the state of a material object is always valid (264). Thus, by virtue of this law of material correspondence, visual information arises.

 

P294. The principle of the appearance of visual information for a quantum of reflected light

Any parameter of a quantum of light reflected from a source of information must necessarily correspond to any parameter of that particular state of its source that existed at a particular moment of this reflection. (3. 2. 2. ) 294

 

Of course, this is not a completely familiar form of research for philosophy. But true principles are reliable supports of knowledge.

 

                GROUP OF SIMULTANEOU S QUANTS

 For a group of simultaneously reflected light quanta, this mechanism works in a similar way. Unless here the connection is considered not of one reflected photon and the source of information, but of a group of simultaneously reflected quanta of light and this source. Moreover, the law of material connection (200) does not prohibit the connection object to be simultaneously in many connections with other material objects.

 

P295

 At the moment of reflection from a material source of a group of simultaneously reflected light quanta, this source and all reflected quanta of a given group are necessarily one material connection. (3. 2. 2. ) 295

                

And since this moment of connection is extremely short, then all objects are in their definite states.

 

P296

Each reflected quantum of light from a group of simultaneously reflected quanta, in an extremely brief moment of its reflection from a source of information, must, like its source, be in their definite states. (3. 2. 2. ) 296

 

  Further, according to the law of the state of material connection (291), any connection is an object capable of changing its states.

 

P297

Each reflected quantum of light, from a group of simultaneously reflected quanta, at the extremely brief moment of its reflection from the source of information, must, like its source, belong to the state of one connection.

                                                                                                        (3. 2. 2. ) 297

 

Since any material connection is one material object (one material system), then all parameters of the state of a material system must necessarily belong to one state matrix. And on this basis, they necessarily correspond to each other.

  

P298. The principle of the appearance of visual information for a group of quanta of the reflected set

At the moment of reflection from a material source of information of a group of simultaneously reflected light quanta, all the parameters of this source and all the parameters of these quanta necessarily correspond to each other.

                                                                                                          (3. 2. 2. ) 298

                  

At first glance, this is an unnecessary repetition of what concerns the reflection of one quantum of light. But these are fundamental truths of information theory, especially since they are still unknown to a wide range of scientists.

 

THE ESSENCE OF THE OCCURRENCE

OF VISUAL INFORMATION

The essence of the resulting visual information is as follows.

 

First, on the one hand, each reflected light quantum necessarily has a specific moment of time of its reflection. This is its physical parameter. This is also his sign. On the other hand, the same specific moment in time is the same for a specific state of the source at the moment of reflection of this quantum. Thus, any reflected quantum carries data on the existence of a specific state of its source of information. This is already mixing.

Secondly, on the one hand, each reflected quantum of light necessarily has a specific place of its reflection. This is its physical parameter. This is also his sign, since he is moving from this place. On the other hand, the same specific place is the same for the state of the source, existing at the moment of reflection of this quantum. Thus, any reflected quantum carries a given about the place of a specific state of its source. This is mixing.

Thirdly, on the one hand, each reflected light quantum has a specific frequency (color). Frequency is its physical parameter. This is also his sign. On the other hand, the reason for its color is the atomic electron of the source. Thus, any reflected quantum carries data on the color of a particular state of the source. This is mixing.

 

Like is cognized by like.

 

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