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				 This section examines the nuclei between hydrogen and carbon12.
				The first step is to examination of the alpha particle. The alpha
				particle is an important nuclear component and is made up of two
				protons and two neutrons that are arranged in a two-layer, six sided
				lattice structure which is composed of six up quarks and six down
				quarks.  
				
				This section on the core continues examining the
				remaining stable nuclei between helium 4 and the third nuclear
				component or first nuclear structure the carbon12 ring. 
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				 Hydrogen comes in three common varieties:  The first two are stable,
				 hydrogen and deuterium, and the third is unstable, tritium. 
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				 A=1  Hydrogen - H1 composed of a single proton. 
				 The proton is made of two up quarks and one down quark. The two
				 'UP quarks' are represented by two black ZOME nodes, and the one 
				 'DOWN quark' is represented by a white ZOME node.  Interconnections 
				 between the quarks in the proton are represented by blue ZOME struts 
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				 A=2  Deuterium - H2 or D2 composed of a
				 proton and neutron. 
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	    When two protons join a positron and a neutrino are ejected to form deuterium 
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				 A=3  Tritium - H3 composed of a
				 proton and two	neutrons. 
				IF, Tritium was like an oreo cooky where the proton was the filling
				 it would have a spin of 3/2.  However, Tritium has a spin of 1/2 
				 so the two neutrons are joined in either a top and side positon or in
				 two side positions.  
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				Helium comes in two common varieties: 
				Helium3 - He3 or Hethree 
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				 A=3   He3 or Hethree is composed of two protons and one
				neutron.  He 3 is the last stable nucleus which contains more 
				protons than neutrons.  Hethree just like tritium cannot be an oreo cooky because 
				the spin would be wrong. 
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				   The possible configurations are the 
				same as tritium just exchanging protons and neutrons. 
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				The nucleus of helium4 is also called an alpha particle. 
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				 A=4  Helium4 - He4 composed of two protons and two
				neutrons. 
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				 Helium4 
				 There are several paths that form helium in the center of stars.
				 For information on these paths can be access at
				           
                Hydrogen Burning in Stars. 			 
				   
				  
				 
				  If access is not available from the original source this file 
				 is available locally at 
				             			 
				  Hydrogen Burning in Stars. (same content in a local file) 	
                  
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				 Following are some possible ways to visualize the structure of the
				alpha by visualizing pseudo growth processes: 
			
				A=4.  
				Two deuterium nuclei can merge to form a helium4 nucleus.
				Helium4 or the alpha particle is a very balanced particle, with
				all the magnetic fields aligned and electric charges in an optimal
				position with respect to each other. The triangular configuration of
				three quarks in the protons and neutrons creates an alpha particle
				that is a flattened six sided structure elongated along one axis.
				The six sided alpha structure plays an important part in the
				building the nuclear lattice structure. As the nuclei of ever large
				elements are formed, it will become apparent that the nuclear
				lattice structure proceeds through distinct phases of The Core, 
				The Star, The Loops, The Extensions and The Island. 
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				A=5 
				
				NONE 
				     
				There is no stable nucleus with an A of five. This is
				the first anomaly along the path of stability. This anomaly occurs
				because the He4 nucleus or alpha particle is so tight and basically
				balanced that He5 does not have the ability to hold on to an extra
				neutron or an single extra proton. So neither He5 nor Li5 exits for
				longer than about 10-22 seconds. 
    	       
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				 A=6  A deuteron can attach itself to one of the ends of
				the alpha particles to make the next stable nucleus lithium Li6. 
				
				Lithium6 can be described as two inter-fingered alpha particles 
				where the central deuteron is common to both alpha's.  In the figure 
				to the left, the left side alpha is formed using a type one alpha bond 
				and the right side alpha is formed using a type two alpha bond. 
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				 A=7  Additional neutron can be added to Li6 capping one of the 
				end protons which creates lithium Li7.  It is not possible to attach 
				an stable additional permanent neutron to the alpha side of lithium
				Li7 and there is no free proton on the deuterium side so there is no
				stable lithium Li8. 
				There is another position where a neutron can fit and the spin will 
				still be 3/2.  That position is a branching off from the center 
				proton to from a star shaped structure. 
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				A=8 
				NONE 
				      
				This is the second gap or anomaly along the path of stability.  
				If a proton is added to the deuterium side of Li7, beryllium Be8 
				is formed which is very unstable. 
				 Why won't or don�t two alphas hold together? 
				    
			   
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				 There are three possible ways for the two alphas to attach to
				each other and each involves four electrical attachment
				possibilities. Thus, a stable linkage is allusive as the two alphas
				try the alternate bonding options. 
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			  Add a neutron to the mix and a spin of 3/2 and an interesting
			 linkage possibility emerges. 
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				 A=9  
				The two alphas couple as four duteriums to form a star attaching the extra neutron
				as a cap over the proton in the central deuteron.  
				The result is beryllium Be9 with a spin of 3/2. 
                      				
				 That extra neutron controls the way the two alphas can bond
				 as four deuterons and thus the Be9 nucleus is stable. 
 
                      
                      
                      
                      
			       
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				A=10  Now add a proton to one of the beryllium Be9 star arms and 
				move the neutron to the end of one of the other star arms. The results is boron
				B10.  Each connection between the alpha arms forms 60 degree angles, and as in 
				all nuclei the ultimate factor controlling structure is spin (magnetic dipoles). 
				
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			  	 Boron 10 and boron 11 have different basic structures.
				  Thus when a neutron is added to boron 10 the result is 
				NOT boron 11. 
				
				  It is easier for boron 10 and a neutron to split 
				into lithium 7 and helium 4 rather than rearrange to form B11.  
				Review the structure of Li7 (A=7) and compare it to the structure 
				of boron 10. 
				Following is a pictorial representation of neutron 
				absorption by boron 10 which forms boron 11 Temp.  The 
				neutron ultimately inducing fission of boron 10 plus a 
				neutron (boron 11Temp) nucleus and why the fission path 
				is more favorable than the path to forming boron 11 
			  
		       
 
                      
                      
 
			    
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                    The tower or stack of 2 protons and 2 neutrons collapses to form 
                    an alpha particle.  The sequence is demonstrated below.  
                      
                      
                      
                      
			   
	
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                      The tower or stack of 2 protons and 2 neutrons collapses to form 
                    an alpha particle.  The sequence is demonstrated below.  
                      
                      
			 
 
                      
			  
			 
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			 Again compare the nuclear structure of boron 10 with boron 11 and lithium 7. 
			
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			           BORON11
			          
			          
			      BORON10 
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			     LITHIUM7 
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				 A=11   There is a gap in the boron B11 partial ring. If
				a Proton and Neutron (Deuteron) fills the gap between two ends and the 
				ring closes to form carbon 12.  
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				 A=12  Finnish closing that ring on B11 with a proton
				and by shifting the neutron down into the same gap to form 
				carbon C12, the next element. This is the carbon ring or
				carbon12 and the structure of this 12-nucleon ring becomes the
				second perceptual structure in the nucleus right behind the alpha
				particle. 
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				Generally a neutron is added before a proton because of the over
				all positive charge on the nucleus. To this point the nucleus grows
				one neutron followed by one proton at a time. This continues for two
				more nuclei while the second carbon ring layer gets started.  After 
				the next two nuclei, nucleon additions occurs in pairs.  Two, four or
				 six neutrons are first added followed by two protons.  For stable 
				 nuclei heavier than oxygen the nucleon are always added in even numbers
				 to maintain stability via balance.   
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