[1] Biler P. Existence and nonexistence of solutions for a model of gravitational interaction of particles. Colloq Mathematicum, 1994, 66: 319-334 [2] Cao X.Global bounded solutions of the higher-dimensional Keller-Segel system under smallness conditions in optimal spaces. Discrete Contin Dyn Syst, 2015, 35: 1891-1904 [3] Gajewski H, Zacharias K. Global behavior of a reaction-diffusion system modelling chemotaxis. Math Nachr, 1998, 195: 77-114 [4] Jia Z. Global boundedness of weak solutions for an attraction-repulsion chemotaxis system with $p$-Laplacian diffusion and nonlinear production. Discrete Contin Dyn Syst Ser B, 2023, 28(9): 4847-4863 [5] Jin C. Global bounded weak solutions and asymptotic behavior to a chemotaxis-Stokes model with non-Newtonian filtration slow diffusion. J Differential Equations, 2021, 287: 148-184 [6] Jin C. Global classical solution and boundedness to a chemotaxis-haptotaxis model with re-establishment mechanisms. Bull London Math Soc, 2018, 50: 598-618 [7] Jin H. Boundedness of the attraction-repulsion Keller-Segel system. J Math Anal Appl, 2015, 422: 1463-1478 [8] Jin H, Wang Z. Asymptotic dynamics of the one-dimensional attraction-repulsion Keller-Segel model. Math Methods Appl Sci, 2015, 38: 444-457 [9] Jin H, Wang Z. Boundedness, blow up and critical mass phenomenon in competing chemotaxis. J Differential Equations, 2016, 260: 162-196 [10] Jin H, Wang Z. Global stabilization of the full attraction-repulsion Keller-Segel system. Discrete Contin Dyn Syst, 2020, 40: 3509-3527 [11] Jin H, Xiang T. Repulsion effects on boundedness in a quasilinear attraction-repulsion chemotaxis model in higher dimensional. Discrete Contin Dyn Syst Ser B, 2018, 23: 3071-3085 [12] Keller E, Segel L. Initiation of slime mold aggregation viewed as an instability. J Theoret Biol, 1970, 26: 399-415 [13] Li J, Ke Y, Wang Y. Large time behavior of solutions to a fully parabolic attraction-repulsion chemotaxis system with logistic source. Nonlinear Anal: RWA, 2018, 39: 261-277 [14] Li X. Boundedness in a two-dimensional attraction-repulsion system with nonlinear diffusion. Math Methods Appl Sci, 2015, 39: 289-301 [15] Li X, Xiang Z. On an attraction-repulsion chemotaxis system with a logistic source. IMA J Appl Math, 2016, 81: 165-198 [16] Li Y. Global boundedness of weak solution in an attraction-repulsion chemotaxis system with $p$-Laplacian diffusion. Nonlinear Analysis: RWA, 2020, 51: 102933 [17] Li Y, Lankeit J. Boundedness in a chemotaxis-haptotaxis model with nonlinear diffusion. Nonlinearity, 2015, 29: 1564-1595 [18] Li Y, Li Y. Blow-up of nanradial solutions to attraction-repulsion chemomtaxis system in two dimensiona. Nonlinear Anal: RWA, 2016, 30: 170-183 [19] Lin K, Mu C. Global existence and convergence to steady states for an attraction-repulsion chemotaxis system. Nonlinear Anal: RWA, 2016, 31: 630-642 [20] Lin K, Mu C, Gao Y. Boundedness and blow-up in the higher-dimensional attraction-repulsion chemotaxis system with nonlinear diffusion. J Differential Equations, 2016, 261: 4524-4572 [21] Lin K, Mu C, Wang L. Large-time behavior of an attraction-repulsion chemotaxis system. J Math Anal Appl, 2015, 426: 105-124 [22] Liu C, Li P. Boundedness and global solvability for a chemotaxis-haptotaxis model with $p$-Laplacian diffusion. Electronic J Differ Equa, 2020, 2020(16): 1-16 [23] Liu C, Li P. Global existence for a chemotaxis-haptotaxis model with $p$-laplacian. Commun Pure Appl Anal, 2020, 19(3): 1399-1419 [24] Liu D, Tao Y. Boundedness in a chemotaxis system with nonlinear signal production. Appl Math J Chin Univ Ser B, 2016, 31: 379-388 [25] Liu D, Tao Y. Global boundedness in a fully parabolic attraction-repulsion chemotaxis model. Math Methods Appl Sci, 2015, 38: 2537-2546 [26] Liu J, Cong W. A degenerate $p$-Laplacian Keller-Segel model. Kinet Relat Models, 2016, 9: 687-714 [27] Liu P, Shi J, Wang Z. Pattern formation of the attraction-repulsion Keller-Segel system. Discrete Contin Dyn Syst Ser B, 2013, 18(10): 2597-2625 [28] Nagai T. Blowup of nonradial solutions to parabolic-elliptic systems modeling chemotaxis in two-dimensional domains. J Inequal Appl, 2001, 6: 37-55 [29] Nagai T. Blow-up of radially symmetric solutions to a chemotaxis system. Adv Math Sci Appl, 1995, 5:581-601 [30] Nagai T. Global existence of solutions to a parabolic system for chemotaxis in two space dimensions. Nonlinear Anal: TMA, 1997, 30: 5381-5388 [31] Nakaguchi E, Osaki K. Global existence of sountions to a parabolic-parabolic system for chemotaxis with weak degradation. Nonlinear Anal: TMA, 2011, 74: 286-297 [32] Nakaguchi E, Osaki K. Global solutions and exponential attractors of a parabolic-parabolic system for chemotaxis with subquadratic degradation. Discrete Contin Dyn Syst Ser B, 2013, 18: 2627-2646 [33] Nirenberg L. An extended interpolation inequality. Ann Sc Norm Super Pisa, 1966, 20: 733-737 [34] Osaki K, Yagi A. Finite dimensional attractor for one-dimensional Keller-Segel equations. Funkcial Ekvac Ser Int, 2001, 44(3): 441-470 [35] Ren G, Liu B. Global dynamics for an attraction-repulsion chemotaxis model with logistic source. J Differential Equations, 2020, 268: 4320-4373 [36] Ren G, Liu B. Global existence of bounded solutions for a quasilinear chemotaxis system with logistic source. Nonlinear Anal: RWA, 2019, 46: 545-582 [37] Shi S, Liu Z, Jin H. Boundedness and large time bahavior of an attraction-repulsion chemotaxis model with logistic source. Kinet Relat Models, 2017, 10(3): 855-878 [38] Tao W, Li Y. Boundedness of weak solutions of a chemotaxis-Stokes system with slow $p$-Laplacian diffusion. J Differential Equations, 2020, 268(11): 6872-6919 [39] Tao W, Li Y. Global weak solutions for the three-dimensional chemotaxis-navier-stokes system with slow $p$-Laplacian diffusion. Nonlinear Anal: RWA, 2018, 45: 26-52 [40] Tao Y, Wang Z. Competing effects of attraction vs. repulsion in chemotaxis. Math Models Methods Appl Sci,2013, 23: 1-36 [41] Tian M, He X, Zheng S. Global boundedness in quasilinear attraction-repulsion chemotaxis system with logistic source. Nonlinear Anal: RWA, 2016, 30: 1-15 [42] Wang Y. A quasilinear attraction-repulsion chemotaxis system of parabolic-elliptic type with logistic source. J Math Anal Appl, 2016, 441: 259-292 [43] Winkler M. Aggregation vs. global diffusive behavior in the higher-dimensional Keller-Segel model. J Differential Equations, 2010, 248: 2889-2905 [44] Winkler M. Finite-time blow-up in the highter-dimensional parabolic-parabolic Keller-Segel system. J Math Pures Appl,2013, 100: 748-767 [45] Yagi A. Norm behavior of solutions to the parabolic system of chemotaxis. Math Japonica, 1997, 45: 241-265 [46] Yu H, Guo Q, Zheng S. Finite time blow-up of nonradial solutions in an attraction-repulsion chemotaxis system. Nonlinear Anal: RWA, 2017, 34: 335-342 [47] Zhang Q, Li Y. An attraction-repulsion chemotaxis system with logistic source. Z Angew Math Mech, 2016, 96:570-584 [48] Zheng P, Mu C, Hu X. Boundedness in the higher dimensional attraction-repulsion chemotaxis-growth system. Comput Math Appl, 2016, 72: 2194-2202 [49] Zhuang M, Wang W, Zheng S. Boundedness in a fully parabolic chemotaxis system with logistic-type source and nonlinear production. Nonlinear Anal: RWA, 2019, 47: 473-483 |