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1 15 Brentwood, TN 37027 USA 37027 TN Brentwood, ,

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and and 1.9 10

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and cosmic gamma rays. gamma cosmic and

[email protected] s NonCommercial - ray emission ray emission of the Q1 which are in similar the structure atomic to the hydrogen - Kwang Hwang -

astrophysical astrophysical observations like the ultra data. It is concluded that the background spectra is o 3.5 keV ray peak observed from x the cosmic x . New can be indirectly seen from the astrophysical observations like t ray Three Three generations of and quarks correspond to the have quarks The charges (LC). charges lepton and (EC) (LC) charges electric the have leptons the Then, work. in the present the EC, LC and color charges (CC). Three heavy leptons and three he to make the missing third eV/c flavor 26.121 of masses of rest the with EC. matters) (dark Then bastons the the as proposed are three (EC) charges new particles which have the electric GeV/c 20 July, 2017 20 July, - mail: mail: Copyright owned by the author(s) under the terms of the Creative Commons the terms Creative of the under the author(s) Copyright by owned -

Speaker 1  Attribution Bexco, Busan, Korea Busan, Bexco, Conference Ray Cosmic International 35th 10

Jae Laboratory JJJ Physics E Cosmic rays and new fermionic dark matters

PoS(ICRC2017)933

, 

nova 1987A 1987A nova - Kwang Hwang Kwang -

Jae , respectively. The, respectively. 2 t b Q3 Q1 Q2 Q3 s s c b d Q2 by the extended standard in the present work. The

t c u d u the astrophysical observations astrophysical the Q1

) ) Quarks(EC,LC,CC) 2 3 5 1 1 0 - - - - - and 42.7 GeV/c LC EC CC 1/3 4/3 2/3

- - 2/3(r 5/3(g 8/3(b) 2 - - -       L L Le L dimensional quantized space space quantized dimensional el and fermionic dark matters el and fermionic ns. But there are no experimental evidences -    e    L

2  e e  e     Le Leptons(EC,LC) anti ) anti 1 2 3 5 anti lepton) anti 0 - - - - LC EC 2/3 5/3 8/3 - -

- - - 5 (3 quarks) (3 5 5 (3 leptons) (3 5

- - prime prime and heavy quarks (T, B, X and Y), sterile e model is introduced as the new extended for - (EC) (EC) luding the new heavy quarks (Q1,Q2,Q3). The super The (Q1,Q2,Q3).quarks heavynew the luding ray peaks are emitted from the Q1 baryon atoms. The rest masses lepton (LC) and color (CC) charges. charges. (CC) color (LC) and lepton -

: LC = : : LC = 0(lepton : B1 B2 B3 Bastons , WIMPS, , preo 5

Baryon: CC = CC Baryon: (quark= 0CC : Paryon Koron The bastons (Dark matters) interact gravitationally but not gravitationally interact matters) (Dark The bastons - EC 2/3 5/3 8/3 -

Dark matters (charge) flavor Each to each corresponds dimensional axis.

- - - . ) and three heavy quarks (Q1, Q2,Q3) are introduced. The rest masses of the high energy cosmic rays are proposed to be originated from the decays and  - nova explosion. - X9 X1 X2 X3 X4 X5 X6 X7 X8 prime boson, W and Y and Total Total Total , L dimensional quantized mod space -

Table 1. Elementary in the three fermions 1. Elementary Table model bastons the because and with the electromagnetically the have do not -  - Three Introduction B1 and B2 dark matters are proposed as 26.121 eV/c In Table 1, the leptons and quarks have the same properties of the Threethree generations. Table In

dimensional quantized spac s, leptons and dark are calculated matters by equations using the simple to show the energy The new physics search beyond standard model has been done -

difference difference between the quarks and leptons is that the quarks have the three color flavors or three color charges (CC) of red (r), green (g) and blue (b) but the leptons do not. The quarks with the generations are called as the lepton charges (LC) or lepton flavors 2. generations separate the leptons and quarks with the same electric charges (EC). Three is discussed in the relation with the B1 dark And . it is concluded that the observed 18.7 3.5 keV and keV, 74.9 keV x of the dark matter core collapse is newly introduced in addition to the normal matter core collapse to explain the super scales. These new particles can be indirectly searched for from the astrophysical observations like observations astrophysical the from for searched indirectly be can particles new These scales. of questions unsolved The rays. gamma cosmic and rays cosmic the Forwork. present the in particles new these of interactions and decays the using byexplained are example, the ultra inc the of annihilations for these new particles. The previously known model have been models developed on the unquantized including space. In the the present work, the string theory three and the the new elementary particles 1 in Tables and 2. The three dark matters (B1,B2,B3), three heavy leptons (Le, L quark 1. models with the new particles. These new particles include the SUSY particles, techniquarks, , Z , X Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic PoS(ICRC2017)933

d 2 when 4/3 and

- -

s build up build s ptons. The ptons. ’ dimensional - Kwang Hwang Kwang - QCD, QCD, 5 for these new 8/3 which make which 8/3 - 3 for the leptons3 for the 1 for the leptons - - - Jae Dynamics, Dynamics, Force, - 5/3 and 5/3 - (0,0,0) Eletro g Quarks (EC,LC,CC) Quarks = F(EC,LC,CC) F(EC)+F(LC)+F(CC) Unobservable force Strong Z/W/Y(EC,LC,CC) Quarks (EC,CC) Quarks Strong Massless (CC) 2/3, the the of - , , ctric charges is ctriccharges zed space of the bastons is in blue in blue in is bastons the of space zed g ) (EC) - Magnetic Magnetic Force - dimensional quantized spaces [1,2]. Each , , W - + 3) of the leptons is decreased by dimensional quantized space in red to the - - (0,0) (Z, (Z, W g Weak force Weak Z/W/Y(EC,LC) (EC) Baryons QED, F(EC), Force Weak bosons Massive Mesons Leptons, (EC,LC)) Baryons = F(EC,LC) F(EC)+F(LC) Normal photon Leptons,

3 dimensional quantized spaces with the summe 1) of the quarks. In Table 1, systematically three - - 2 for the third missing electric charges are added to - dimensional quanti dimensional

- dimensional quantized space in green to the le the to green in space quantized dimensional - arated with three color charges (CC). Because the lepton (EC) dimensional quantized spaces in red and in blue in 1. Table the present extended standard model are compared [1,2]. are compared model standard extended the present -

5. The three - Dynamics, EM Force: Electro Dynamics, Force: EM - (0) are expected. The sum of three electric is charges g Dark force Dark matter Z/W/Y(EC) Bastons (Dark matters) F(EC), dimensional quantized spaces in green, in red and in blue 1. in Table - e made by adding the three 1 are colored in blue, red and green, respectively in Table 1. Let 1. Table respectivelyin green, and red blue, in colored are 1 dimensional Quantized Space Model, QED: dimensional Quantum Quantized - - 1 in Table 1 1. Therefore, in Table the heavy quarks with 1. First, the new heavy leptons and new heavy quarks have the electric charges charges electric the have quarks heavy new and leptons heavy new the First, 1. - - (TQSM) 3 and 3 - 1/3 for the quarks. The electric charges are quantized on the basis of the - Standard Model, ESM: Extended Standard Model, Model, Model, Standard Extended ESM: Standard 5, - 4/3, respectively in Table 1. Then the sum of three ele of three sum the Then 1. Table in respectively 4/3, dimensional quantized spaces of the leptons and quarks from the three - Table 2. Standard model and model 2. Standard Table - SM: Three TQSM: QCD: Chromo Quantum (LC) not is considered. the charges to lepton corresponding In SM, the force (EM Force), Photon (EM Force), QED Short Force Range bosons Massive (EM Force), Photon (EM Force), Short Force Range ESM Force Long Range SM Long Force Range 1 for the quarks. The summed electric charge ( e new concepts. Only the electric charges have been quantized on the basis of the electron the same lepton charges are separated with two electric charges of 0 and - 2 and - the quarks are made by adding the three the adding by made are quarks the lepton charges of the quarks are the same as the electric charges of the leptons and the color quantized space of the bastons. The three The bastons. the of space quantized 1. Table The leptons have the three The quarks have the three Therefore, the leptons ar And bastons. the of charges electric the as same the are leptons the of charges lepton The bastons. particles particles called as the bastons are bastons the for charges electric The bastons. as called particles the summed electric charge of of charges the three on th of charge electric of and compared with the summed electric charge ( complete the three flavors of EC, LC and CC in the quarks and leptons in Table 1. The elementary The 1. Table in leptons and quarks the in CC and LC EC, of flavors three the complete 1 can be explained only by the three Table fermions in flavor corresponds to each dimensional axis in 1. Table. This work needs the further researches charges charges and color charges have the three flavors, the electric charges are expected to have three the flavors. But the electric charges of the leptons and quarks have two flavors. The particles with and 2/3 and electric charge of heavy leptons with the electric charge of Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic same charges of EC and LC are sep PoS(ICRC2017)933

- - he the ray tive -

So it So

5]. 5/3 and - m m the pair ray peaks are Kwang Hwang Kwang 2/3, - - - 2. For example, - Jae ray energies ray are energies 18.7 ray peak is expected June 2011 [1, 2011 June

ray peak is seen more seen is peak ray - - - - 1 and not electromagnetically - ray background spectra

ray supports the presence the supports ray - -

8/3. Therefore, the leptons the Therefore, 8/3. - e charge configurations of ic x m burst in May in burst 5/3 and 5/3 - - 2 for the quarks and -

, respectively [1,2]. It is called as t - out

2/3, 6]. So it is thought that this observed 3.5 observed this thoughtthat is it So 6]. - 1 and - X(INTEGRAL) data in its bright state - 4]. And the 74.9 keV x keV 74.9 the And 4]. ray pulsar 4U 0115+63 from IBIS/ISGRI and

- 4 harges of the elementary fermions can be assigned be can fermions elementary the of harges baryons to form the Q1 baryon atoms. These Q1 baryon atoms are similar to the hydrogen atoms. The energy levels in the Q1 baryon atom are easily calculated in the electron energy same levels in the way hydrogen atom are as Thecalculated. calculated x keV and 3.5 keV from the R atom and 74.9 keV and 13.9 keV from the Q atom possible in 18.7 keV and Fig. 74.9 keV 1. x The found at the cos [1,3, clearly on the broadband energy spectrum of the X JEM the during x and 74.9 keV is thought 18.7 that these keV peaks are originated the in from Q1 atoms baryon Fig. 1. Also, the 3.5 keV x (EC,LC) = (1,0) can rotate around these Q and R rays and Q1 baryon atoms - quarks are quarks

4//3 in Table 1. Table 4//3 in -

m. m. - ray Background using a total of 10 Ms Chandra observations - quarks because the leptons do not have the color (CC) charges. rays in the in the rays -

m for the R atom for the R atom m 14 - Legacy and CDFS survey fields [ surveyfields CDFS Legacyand 1,0), respectively. Then the protons with th - ) is 2.9 10 ) is m for the Q atom. The half The Q atom. for the m 1

14 - 3.5 keV, 18.7 keV and keV x 74.9 3.5 keV, ray peak is originated from the Q1 baryon atom of the R atom but not fro arks should be described as (EC,LC) and (EC,LC,CC), respectively as shown 1. in Table spectrum of the Cosmic X - The heavy baryons including the Q1 heavy quark (Q1 baryons) can be made in the ac

Q1 baryon atoms of the R atom and Q ato of the R atom atoms Q1 baryon (r The radius 10 and 1.4 be can quark Q1 and baryon Q1 of the lives the xrays. emit to long enough Fig. 1. Proton energy levels and x and levels energy Proton Fig. 1.

in the COSMOS the towards keV x x cosmic 3.5keV the of presence The matters. dark the of annihilation ofof the Q1 withquark charge the electric from from the Q1 baryon atom of the R atom in And Fig. an 1. emission line at 3.5 keV was detected the Q(Q1,d,d) and R(Q1,d,u) baryons in Fig. 1 have the charge configurations of (EC,LC) = ( 2,0) and(EC,LC) = ( hadronization. 3. galactic nucleus. This Q1 baryon can have the electric charges (EC) of with the electrons,and protons quarks the bastons because do nothave the lepton (LC) and color but gravitationally interact leptons the Also, matters. dark the are bastons the Then, charges. (CC) not electromagnetically with the of hadrons the because protons like hadrons the with electromagnetically interact can leptons The the mesons and baryons have the color charges of 0 and the bastons in Table 1. Therefore, all quantized c quantized all Therefore, 1. Table in bastons the 1.as Then, theshown lepton in Table charges are 0, for charges color the And leptons. the for 8/3 and qu as same the properties the have particles new These (EC). as described are bastons the Therefore, the dark matters have. These new particles interact gravitationally but Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic of charges electric leptonsthe the and of the lepton as charges same the quarksare the of charges PoS(ICRC2017)933

e F  

- and

  eV and

ray. The ray. - 17 LAT. This LAT. for Q1,Q2 for -

2 e and B1 eV for eV - t the rest mass rest the t

Kwang Hwang Kwang

- 5 - 2

9 8 15 Jae

5 10 when the 10 10 10

(eV) . ]. The 42.7peak]. GeV  2  calc calc ]. ]. And the 26.121 5.11 E 4.27 1.777 10 1.057 10 1.948 , 5.94710 e eV, E(Q2) = 7 10  and

the rest mass of the B2 dark

9 8 5 e 15 10 

10 (eV) ? ? And the rest mass energies of the

eV for for eV exp + 2.14 |LC| + 0.005 LC 0.005 + |LC| 2.14 +

5.11 10 E 7 4.27 1.777 10 1.057 10 2 - . . Then,

) ) can be calculated in Table 3. And the ray spectrum from the Fermi Large Area Large Fermi the from spectrum ray

-  5/3) 2/3) 8/3) - 2/3) 5/3) 8/3) - - , L + 0.62683|LC| + 0.22755LC+ - - -

1, (dark (dark matters) are compared with the experi- 1, 1,  2 in Fig. 3 -

- -

( ( B1( B2( B3( (EC,LC)

 e(  The calculated rest mass energy of the B1 dark

5 ]. are assumed to be negligibly small. Then E = 10

1 dark matters produced from the LHC accelerator. accelerator. LHC the from produced matters dark 1

1 7 5 - - - 13 15 18 enhanced intensity was observed foraround 42.7 GeV c ray spectra, respectively [1,7 assive nearby Galaxy Clusters [8

(eV)

eak [9 1.13858EC

calc calc - E 2.876 10 5.947 10 1.000 10 8.811 10 2.533 10 5.239 10 dark matters) high energy cosmic rays cosmic high energy -

. And the . 14

- 2

16.01455|EC| + 15.02553 EC 15.02553 + 16.01455|EC|

exp ? ? ? ? ? 12 - E (eV) 10

anti B2 annihilation peak

high energy cosmi - – 5/3) 2/3) 8/3) 5/3) - 8/3) 2/3) - - - - - ) = 0.1 eV. in Table 3. It in will Table be interesting to confirm these rest mass energies of three  eV for bastons ( 2, 2, 2,

- - -  eV for leptons  anti B2 annihilation p (0, C) are calculated by using the simple equations under the assumptions of E(B2) of assumptions the under equations simple the using by calculated are C) ( (0, (0, (

 e   

 (EC,LC) ed by fitting the experimental rest mass energies. Then, the unknown neutrino

   – L Le( L

calculated and compared with the experimental values [1]. E=mc values [1]. experimental the with compared and calculated Table 3. Rest masses of the leptons and bastons(dark matters) are are matters) bastons(dark and the leptons of masses 3. Rest Table 38+2F 2 38+2F eV. 23.24488 + 7.26341|EC|

- 20 eV foreV

1 - Originsof high and ultra The The dark matters can interact with the leptons as shown in Fig. 2. The B1 The 42.7(7) GeV peak was identified in the gamma the in identified was peak GeV 42.7(7) The

calculated restcalculated of three neutrinos energies mass are 2.876 10 1.000 10 neutrinos 3. in The Table rest masses of the elementary fermions depend on both of EC and LC Telescope (LAT) in the directions of 16 m (LAT) Telescope is proposed as the B2 matter is 42.7(7) GeV/c Fermi the with measured as W44, (SNR), remnant supernova of spectra ray gamma the might be the B It will be interesting to peak at the look x for cosmic the 26.121 eV is 26.121matter eV. effects effects on the rest mass energies of the quarks 10.34076 = F(EC,LC) and eV and Q3 quarks. The obtained rest mass energies are E(Q1) = 5 10 E(Q3) = 10 order to show the energy scales of these particles by using the simple equations. The parameter values are assign masses and the masses of the heavy leptons (Le, L tha assumed is it Also, too. calculated, be can matters dark B3 and B1 the of masses energies of Q1, Q2 and Q3 quarks correspond to the energies of the first knee, second knee and ankle parts of the ultra mental values in Table 3. The rest mass energies of the leptons and dark matters are calculated in calculated are matters dark and leptons the energiesof mass rest The 3. Table valuesin mental Only the EC and LC charges of the leptons and bastons are used for the calculations of the rest masses. The rest masses of the leptons and bastons leptons with the charge configuration of (EC,LC) and (E bastons of configuration (dark matters) with the charge = 42.7 GeV and E( F(EC,LC) = E = 8.1365 10 E = 17.150110 interactions in Fig. 2 can enhance the electrons numbers and get of through the thedense dark matter cosmic clouds near the galaxy Also, center. the B1 dark matters can be produced from the The LHC observation accelerator. of the enhanced B the of evidence indirect the be will neutrinos The LHC and cosmic neutrino experiments will be interesting. Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic 4. PoS(ICRC2017)933

] ] - ]. in

14 [10 -

2. The elec- high energy - - , respectively. , respectively. Kwang Hwang Kwang spectra can be -

ted ted from the Le + g the Q1, Q2 and Jae ]. ]. It is assumed that asar V404 Cygni V404 asar 5/3 has the rest mass ons as shown in Figs. - in Fig. 3 2. The B3 dark matter with HESS and Fermi and HESS with

- qu - by the inelastic Comptonby the inelastic 3946 - energy energy cosmic ray spectra [1,7

2 which have the ultra

anti B2 annihilation peak is at 4.27 - high

are separated into three groups. First ]. eported in several references [11

- - decays - eV. And the smooth background curve eV. eV) is consistent with the energy of the of energy the with consistent is eV)

cosmic cosmic electron and spectra at

and the heavy lept

13 1 which have the The high range. energy 13 2 - is the rest mass energies of the particles. of the energies mass is the rest high energy cosmic ray spectra is caused by

eV consistent with the rest mass energy (5.11 (5.11 consistent with the energy rest mass eV - 2

eV/c , the B2 6 c

]. The astrophysical neutrino observed spectra ]. at 20 6 - 15 2 10 18 2/3 has the rest mass energy between the first group first the between energy mass rest the has 2/3 E=m 1 and third group with EC=

eV. The eV. positron anomaly, e and e - high energy cosmic rays with the energy higher than higher energy the with rays cosmic energy high - -

- – hadron and Q3

using the Q1 hadron decays [1,15 anti Le annihilation peak was identified at the energy leptons with EC= 15 - 5

high energy cosmic rays are mostly composed of the

1. The B2 dark matter with EC= - –

 - ]. These protons are accelerated protons are accelerated These ]. Le [7

and L

 decays [1,16 hadron, Q2 - , L Le

spectra can be found[7,19 in Ref.

e annihilation peak is at 2.53 10 gamma rays emitted from the pair annihilations of Q1, Q2 and Q3 hadrons. calculated rest mass energy (2.534 10 (2.534 energy mass rest calculated anti L

smic smic gamma ray spectra in Fig. 3 ]. ]. It can be confirmed from the observed – the eV in the TeV gamma ray spectrum from RXJ1713.7 from spectrum ray gamma TeV the in eV

]. ]. . The B1 dark matter with EC= with matter dark B1 The . 17 14 - - ]. The ]. 12 8/3 has the rest mass energy similar to those of the third group with EC= - in Fig. 3 Fig. in . These cosmic electron, positron and neutrino spectra are mainly origina For the co

y between the second group with EC= Fig. Fig. 2. B1 dark matter are compared. particles elementary and lepton interactions to give the neutrino enhancement. New positron annihilation peaks associated with the outburst of the micro the of outburst the with associated peaks annihilation positron eV eV and Le

- eV eV are originated from the decay and annihilations of the hadrons includin eV) of the electron. The possible gamma inducedgamma protons3 in Fig.

10 9 5 are explained by using the Q1 The observed ray cosmic the decays of other heavy leptons and heavy hadrons have the relatively small contributions when contributions small relatively the have hadrons heavy and leptons heavy other of decays the compared with the Le decays. The ultra protons. The smooth background curve of the ultra the scattering with And the first knee, second knee and ankle parts of the ultra Fig. 3 decays [1,15 the energy TeV And range. the cosmic electron, positron and neutrino spectra coming from the Q1 hadron decays are added around 5 10 explained bythe Le and anti the PeV energy range can be explained by 10 shapes These decay. Le the from emitted rays gamma the by caused are rays gamma cosmic the of of the cosmic gamma ray spectra have been observed and r origins same the have spectra ray cosmic the neutrinos, and electrons, cosmic the For range of 10 of range [11 data Lat ultra and high The 3. Table in peak observed 10 Q3 quarks with the possible rest masses of 10 4 and 5 [12,13 with EC= tron range identified of4 were 10 at the energy 10 group is made of the three neutrinos with EC=0 which have the low range. energy Second group is made of the electron, and lepton with EC= third group is made of the Le range with EC=0 and second group with EC= energ Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic according to the above mass energy equations. The leptons PoS(ICRC2017)933

- he ) is and

 nova 2 - neutrino 22]. 22]. T - - nova struc- - Kwang Hwang Kwang - of the dark mat- dark the of nova 1987A anti 1987A nova - Jae of EC andof EC LC. New

can be drawn as shown in shown as drawn be can urve A fits other data well data other fits A urve

are extracted from the an-

nova 1987A [20 1 dark matters coming from coming matters dark 1 2 anti B1 dark B1 anti � - nova 1987A has been seen to seen been has 1987A nova - - 퐵 erimental erimental neutrino measure-

. The neutrino energy of E( pair. annihilated within the earth atmos-

-  The super The have the three rings space telescope on pictures. And the evi- the Hubble dence of the star is missing in the super neutrino masses of 21.4(12) eV/c 4.0(5) eV/c tineutrino data from These [20]. neutrino the masses 1987A are super too large. So, I tried to solve these two questions by using the B1 dark matter. concept new Then, the ter core collapse in addition to the nor- mal matter core collapse is introduced in order to build the super ture. The experimental in conclusions the draw to used are data anti the present work. The more details on the exp references the from found be can ments super The [20,21,22]. data neutrino Fig. 4 anti anti

isused [20]. The c The [20]. isused 

0 t 4

c nova 1987A. The B1 The nova 1987A. 2 7 - t = m = t 2 ) of the observed neutrinos are similar to the energies,

 the the neutral boson (Z(0)) interactions with p and e in the

E( 1 dark matters are pair

� high energy high energy - 퐵

pair is created. These neutrinos are observed by using the detectors dimensional quantized space model is introduced as the new extended new the as introduced is model space quantized dimensional

� - 휈 . Neutrino data of the super data of the Neutrino .

Fig. 4 the create to pair is annihilated matter and anti

 . Origins of the high and ultra high and of the Origins . Summary 3 the earth surface. The energies In summary, the three the summary, In Fig. rays. gamma and rays cosmic

particles particles of bastons with only one charge of EC are the And dark the matters. rest mass energies charge the with matters) (dark bastons and (EC.LC) of configuration charge the with leptons the of matter is 26.12matter eV. 5. standard model. Three generations of the leptons and quarks correspond to the lepton charges. of EC, LC CC, andQuarksand have leptons threehave two charges charges phere and the under E(B1) of the B1 dark matters. This supports indirectly that the rest mass energy of the B1 dark the SN1987A change the directions by earth atmosphere. The B1 and anti related to the time of t. The equation of 2E of equation The t. of time the to related except the uses 6 data. the A The proposed curve dark matter mass of B1. It is proposed that the anti and B1 The earth. the to 1987A SN the from come particles B1 Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic PoS(ICRC2017)933

L It

- ray - high - data. data.

A 8 (2016). - 31 (2017), - . It is thought Kwang Hwang Kwang 2 - raybackground - Jae eV/c

, October 2 , October 20 - , January 28 , January 15

. .

2017

in Table 3. And the calculated the And 3. Table in

 ray and at LHC. The ultra The ray and at LHC. and annihilations of the hadrons the of annihilations and  - supported by the SN1987

n/313247136

eV for eV

. 1 .

- . 1

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(2003) .

375

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21 eV 21 eV

rs/nnp/cr.html. . 777 and 1.000 10 1.000 and

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103525 (2013) 625 sing the simple equations. The standard model has the charge. charge. However, the present model has only one

- (2014) (2014) 121102 (2014)

. 39

113 113 . . A49 (2016) (2012)

and x eV for for eV Also, see Refs. [23,24]. .psu.edu/use

the pair annihilations of the dark matters but from the x Phys. Lett. Phys. 5

93 - 35 . D

(2010)

Talk at Intl. Conf. on New trends in high energy physics energy in high trends on New Conf. Intl. at Talk 512 Talk at American physical society April meeting April society physical American at Talk

https://www.researchgate.net/publication/314246000 https://www.researchgate.net/publicatio , 5.947 10 5.947 , Phys. Rev. Lett Rev. Phys. Phys. Rev. Lett Rev. Phys. e Astronomy Letters Astronomy Phys. Rev. Phys. arXiv: 1008.4726v1 (2010). 1008.4726v1 arXiv: arXiv: 1603.01169 (2016). (2016). 1603.01169 arXiv: 

A&A The Astrophysical Journal Astrophysical The i, arXiv: 1412.7639 (2014). 1412.7639 i, arXiv: t al., al., t arXiv: 160407584v1 (2016) 160407584v1 arXiv: Astropart. Phys Astropart. , arXiv: 1608.02018 (2016) and references there in. there references and (2016) 1608.02018 arXiv: eV for eV

7

- Kwang Hwang, Hwang, Kwang Hwang, Kwang - - Kwang Hwang, Hwang, Kwang Kwang Hwang, Hwang, Kwang - - https://absuploads.aps.org/presentation.cfm?pid=12521 Jae et al., Turler M. et al., Shi Yong e Boldin P.A. (2017). 1701.07932 arXiv: et al., N. Cappelluti (2013). 1301.6619v1 arXiv: S. Hussain, Jae Y.F. Liang et al., al., et Liang Y.F. ] M.G. Aartsen et al., arXiv: 1412.5106 (2014). 1412.5106 arXiv: al., et Aartsen M.G. ] et al., Accardo L. ] al., et Aguilar M. ] ] T. Siegert et al., Siegert T. ] www2.astro et al., Meszaros P. ] Waxman, E. and Bahcall J.N. ] (2015). 1502.06355v1 arXiv: et al., Federicici S. ] ] V. Gammald V. ]

] M. Ackermann et al., arXiv: 1302.3307v1 (2013). 1302.3307v1 arXiv: et al., Ackermann M. ] [21] F. Vissani et al., Vissani [21] F. (2015). 1507.07107v1 arXiv: Schatz, [22] G. [23] Jae [24] Jae [15 [16 [17 Lipari, [18] P. Dova [19] M.T. [20] R. Ehrlich, [8] [9 [10 [11 [12 [13 [14 [2] [3] [4] [5] [6] [7] [1] est mass ofenergy the B1 dark matter is 26.1

spectra are originated not from emission of Q1 the baryon atoms. References r x peak cosmic at the eV 26.121 the will be for to look interesting decay the from originated are rays gamma and rays cosmic energy including the Q1, Q2 and Q3 quarks with the possible rest masses of 10 x x raycosmic observed the peaks from 74.9 andkeV keV 3.5 keV, 18.7the that conservation rules of many quantum numbers such symmetry, as hyper baryon charge, number, weak lepton charge, number, electric B charge, number, color lepton charge, family quark flavor number neutrinos three of energies mass quantum rest calculated The charges. CC and LC EC, of rule conservation 10 2.876 are Cosmic rays and new fermionic dark matters dark fermionic new and rays Cosmic configuration of (EC) are calculated by u