Original articl the scalar unparticle production from the collision process in unparicle physics

VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 7 Original Article  The Scalar Unparticle Production from the Collision Process e  in Unparicle Physics Le Nhu Thuc*, Dao Thi Le Thuy Hanoi National University of Education (HNUE), 136 Xuan Thuy, Cau Giay, Hanoi, Vietnam Received 24 September 2019 Revised 04 November 2019; Accepted 15 December 2019 Abstract: The production of scalar unparticle (spin - 0) in the photon - electron ( )e  collider is calculated in all s-, t-, and u-channels in detail as well as interference between channels together. By searching for missing energy distributions as well as evaluating dependence of differential cross section (DCS) on the scattering angle ( ) and cross section (CS) on the center of mass energy ( )s , we hope that the unparticles production in high energy collider might be detected in future. Keywords: Scalar unparticle, photon-electron, DCS, CS. 1. Introduction The attractive scenario for describing a possible scale-invariant hidden sector with a continuous mass distribution, which is described in terms of “unparticle” was proposed by Georgi [1]. This scale - invariant sector combined with the Standard Model through interactions of the form UVSM, where UV is an unparticle operator and SM is a Standard Model operator. A concrete example which can support unparticle stuff was suggested by Banks-Zaks [2, 3], with a suitable number of massless fermions, theory attains a non-trivial infrared fixed point and a conformal filed theory can be realzed at a low energy [4]. The Lagrangrian of the uparticle physics is as follows [4] ________ Corresponding author. Email address: thucln@hnue.edu.vn https//doi.org/ 10.25073/2588-1124/vnumap.4384 L.N. Thuc, D.T.L. Thuy / VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 8 4UV n d n c L M    UVSM, (1) Where M is the energy scale characterizing the new physics, the operatorUV and operatorSM have dimension dUV and n, respectively and cn is a dimension-less constant. In the low energy effective theory, the form of the operator is: 4 UV U UV d d U n d n L c M      USM, (2) Where the unparticle operator U with a dimension dU. In this paper, we calculate in details the production of scalar unparticle in the photon – electron ( )e  collider in all s-, t-, and u-channels. Evaluating the dependence of the DCS on the scattering angle ( ) , we have shown the relevant direction to be able to observe unparticles. In addition, the CS are also considered as a function of the center of mass energy ( )s . 2. The process 0spine U e    in unparticle physcis The corresponding Feynman diagrams for the pair production of unparticle and electron in e  collider are shown in Fig. 3.1. Fig 3.1. The Feynman diagrams for the process Uee   According to the Feynman rules we calculate the amplitude squares of the s-, t- and u- channels as well as the interference between channels together. The resulting expressions are as follows: 2 2 2 2 2 20 1 2 1 2 21 2 2 8 { [2( )( ) ( )] 4 ( ) 2 ( )U s s s s l s l sd U s l e M p q k q q p k m k q m q q m               L.N. Thuc, D.T.L. Thuy / VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 9 4 2 2 2 2 4 2 2 2 2 2 1 1 2 2 1 22 2 ( ) ( ) 2 ( ) 2 [2( )( )l U s l s U s l U s s l U s sm q m p q q p k m q k q m p q k q            2 2 2 4 2 2 2 2 41 2 1 1 2( ) ] 2 2 ( ) ( ) 2 }s l U s l U s s l lp k q m q m p q q m p k m         , (3) 2 2 2 2 20 1 2 1 2 2 1 21 2 2 8 { [2( )( ) ( ) ] 2 ( ) ( ) ( )U t t t t l t ld U t l e M p q k q p k q m k q m p k q m               2 4 2 2 2 2 2 2 1 2 2 1 2 1 2( ) 2 ( ) [2( )( ) ( ) ]U t l U t t l U t t tq p k m q k q m p q k q p k q         2 2 2 4 2 2 4 2 2 2 4 2 21 12 4 ( ) 2 2 4 ( ) 2 }l t l t l l U t l U t t l U tm q m p q m m q m p q q m q            , (4) 2 2 20 2 1 2 1 2 2 2 2 2 2 12 4 4 {2[( ) ( ) ( )( )( ) ( )( )( ) U u u u u u ud U u e M q p p k p p q k q p q p p k q p q          2 2 2 2 1 2 2 2 2 1 2 2 2( )( ) ] 2[ ( ) ]( )( ) ]}u l u u up p p k q k p m q p q p p q     . (5) The expressions when there are interference of channels as follows: 2 2 1 2( 1) 2 2 2 2 8 ( )( )U s t d U l t l e M M q m q m        2 2 2 1 2 2 1 2 2{2( )( ) ( ) ( ) 2 ( )t s l t l l sp q k q m k q m p k m k q    2 2 2 2 2 2 1 2 2( )( ) 2 ( )U t s s s l U s tq q p q q k m k q q     2 2 2 2 2 2 2 2 4 1 2 2 1 12 ( )( ) ( ) 2 ( ) ( ) ( ) 2l U t s l U s t l t l s t l s lm p q k q m q k q m p q m q q m p q m          2 2 2 2 2 2 2 2 2 2 4 2 1 1( ) 2 2 ( ) ( )}l U s t l U s t l U t s l U s tm p q q m q q m p q q m q q            , (7) 2 2 10 2 1 2 2 2 16 ( )U s u Ud U s l u e M M q m q         2 2 2 2 2 2 1 2 2 1( ){ 2[( ) ] 4 ( ) 4 2 ( )}u s l s l s l sq p p k q m q k m q m p q     2 1 2 2 1 2 2 1 2 2{ [( )( ) ( )( ) ( )( )]s u u uq p q k p p k q p p p k q   2 2 2 2 2 2 2[( )( ) ( )( )+( )( )]l u s u s u sm q q k p q k q p q p k q  2 2 2 2 1 2 1 2 1 2( ) [( )( ) ( )( )+( )( )]}l u s l u s s u s um q p q m p q q p p q q p p p q q   , (8) 2 02 1 2 1 2 2 2 16 ( )U t u Ud U t l u e M M q m q         2 2 2 2 1 2 1 2( ){ 2( )( ) 4 ( ) 2 ( ) 4 ( )}u t t l t l t l t tq p q q p k m p q m q k m q q     2 1 2 2 1 2 2 1 2 2{ [( )( ) ( )( ) ( )( )]t u u uq p q k p p k q p p p k q   2 1 2 1 2 1 2[( )( ) ( )( ) ( )( )]l t u u t t um p q q p p q q p p p q q   2 2 2 2 2 2 2 2 2[( )( ) ( )( ) ( )( )] [( )( )]}l t u t u t u l t t um q q k p q k q p q p q k m q q q p    . (9) From these expressions, we evaluated the number of DCS, CS and discussed ability to produce unparticle in the next section. L.N. Thuc, D.T.L. Thuy / VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 10 3. Numerical results and discussions To estimate the numerical values and examine the DCS and CS, we choose 0 1  ; 1 1  ; 1.7Ud  ; 1U TeV  [5] and 3000s GeV . From the square of matrix elements above, we evaluate the (DCS) as a function of cos by the expression: 1 2 1 1 cos 64 kd M d s p     . (10) the results are shown in figure 3.2. a) b) b1) c) c1) d) Fig 3.2. The DCS as a function of cos L.N. Thuc, D.T.L. Thuy / VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 11 From the figure 3.2, we see that: for s - and t - channels (fig 3.2 a and fig 3.2 b) the DCS reaches the maximum value ( 52.24 10  pbarn for s channel and 46.4 10  pbarn for t channel see fig3.2b1: the fig 3.2b1 is magnified from figure 3.2b in the range of cos from 0.9 to 1) if the direction of the particle produces the same direction of the particle at the initial state, while the u- channel (fig 3.2c and fig 3.2c1: the fig 3.2c1 is magnified from figure 3.2c in the range of cos from -1 to -0.8) is the opposite, the direction of particle generated in reverse with the direction of the particle at the initial state, the DCS has the maximum value: 324 10  pbarn (fig 3.2 c1). However, when the phase is associated with all s-, t- and u- channels, the DCS is shown in fig 3.2d, we can see that the DCS has a divergence at cos 1  , and the major contribution to the DCS is on u - channel and t – channel. Fig 3.3. The CS as a function of s In Figure 3.3, we plot the integrated DCS versus the s with 500 3000GeV s GeV  . The CS decrease sharply while s increases from 500GeV to 800GeV for the s- and t- channels (fig 3.3 and fig 3.3 b). Similarly, the CS in the case of associating with all s-, t- and u- channels (fig 3.3 d). However, it decrease steadily in the range s from 800GeV to 3000GeV . Especially, for u– L.N. Thuc, D.T.L. Thuy / VNU Journal of Science: Mathematics – Physics, Vol. 36, No. 1 (2020) 7-12 12 channel only, the CS increases drammatically while s increases from 500GeV to 1500GeV , then increases slightly in the range s from 800GeV to 3000GeV (fig 3.3 c). 4. Conclusions The cross sections of the pair production of scalar unparticle e  collider depend significantly on the scattering angle and the center of mass energy. We have found the relevant direction to be able to detect unparticles, which the direction of the particle produces the same direction of the particle at the initial state. In addition, the total cross sections increases sharply while s increases from 500GeV to 1500GeV for u-channel only. This results may be contribute to experiment in researching unparticles. References [1] H. Georgi, Unparticlephysics, Phys. Rev. Lett. 98 (2007) 221601. [2] T. Banks, A. Zaks, On The Phase Structure Of Vector - Like Gauge Theories With Massless Fermions, Nucl. Phys. B 169 (1982) 189. [3] V. Khachatryan and et al, Search for dark matter and unparticles produced in association with a Z boson in pp collisions at 8s TeV at CMS”, Phys. Rev. D 93, (2016) 052011. [4] T. Kikuchi, N. Okada, Unparticle physics and Higgs phenomenology, Phys. Lett B 661 (2008) 360-364. [5] K. Cheung, W.Y. Keung, T.C. Yuan, Collider Phenomenology of Unparticle Physics, Phys.Rev.D76 (2007) 055003.