∗ | a | b | c |
a | a | b | a |
b | b | b | b |
c | a | b | c |
In this paper, a two-grid mixed finite volume element (MFVE) algorithm is presented for the nonlinear time fractional reaction-diffusion equations, where the Caputo fractional derivative is approximated by the classical L1-formula. The coarse and fine grids (containing the primal and dual grids) are constructed for the space domain, then a nonlinear MFVE scheme on the coarse grid and a linearized MFVE scheme on the fine grid are given. By using the Browder fixed point theorem and the matrix theory, the existence and uniqueness for the nonlinear and linearized MFVE schemes are obtained, respectively. Furthermore, the stability results and optimal error estimates are derived in detailed. Finally, some numerical results are given to verify the feasibility and effectiveness of the proposed algorithm.
Citation: Zhichao Fang, Ruixia Du, Hong Li, Yang Liu. A two-grid mixed finite volume element method for nonlinear time fractional reaction-diffusion equations[J]. AIMS Mathematics, 2022, 7(2): 1941-1970. doi: 10.3934/math.2022112
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In this paper, a two-grid mixed finite volume element (MFVE) algorithm is presented for the nonlinear time fractional reaction-diffusion equations, where the Caputo fractional derivative is approximated by the classical L1-formula. The coarse and fine grids (containing the primal and dual grids) are constructed for the space domain, then a nonlinear MFVE scheme on the coarse grid and a linearized MFVE scheme on the fine grid are given. By using the Browder fixed point theorem and the matrix theory, the existence and uniqueness for the nonlinear and linearized MFVE schemes are obtained, respectively. Furthermore, the stability results and optimal error estimates are derived in detailed. Finally, some numerical results are given to verify the feasibility and effectiveness of the proposed algorithm.
The notion of a neutrosophic extended triplet group (NETG), as a new generalization of the notion of a standard group, is derived from the basic idea of the neutrosophic sets. The concept of neutrosophic sets [8], first introduced by Florentin Smarandache in 1998, is the generalization of classical sets [9], fuzzy sets [13], intuitionistic fuzzy sets [1,9] and so on. Neutrosophic sets are very useful to handle problems consisting uncertainty, imprecision, indeterminacy, incompleteness and falsity. As a result, neutrosophic sets have received wide attention both on practical applications [5,6,7] and on theory as well [14,15].
Since groups are the most fundamental algebraic structure with respect to some binary operation and play the role of back bone in almost all algebraic structures theory [2,3,10], Smarandache and Ali introduced the notion of a neutrosophic triplet group (NTG) [12] as an application of the basic idea of neutrosophic sets. A semigroup (N,∗) is called a neutrosophic triplet group, if every element a in N has its own neutral element (denoted by neut(a)) different from the classical identity element of a group, and there exists at least one opposite element (denoted by anti(a)) in N relative to neut(a) such that a∗neut(a)=neut(a)∗a=a, and a∗anti(a)=anti(a)∗a=neut(a). Here, since neut(a) is not allowed to be equal to the classical identity element as a special case, the notion of a neutrosophic extended triplet group (NETG) was introduced in [11] by removing this restriction, and so the classical groups can be regarded as a special case of NETGs. Until now, much research work has been done on NTGs and NETGs [4,16,17,18,19,20,21] and many meaningful results have been achieved. Similar to the role of subgroups played in group theory, the notion of NT-subgroups is also an important basic concept in NETG theory, which has been proposed in some literatures (see [16,17]). To further study structures of NT-subgroups, in this paper, we shall consider (prime) ideals on NETGs, which are a special kind of NT-subgroups.
This paper is organized in the following way. In Section 2 we will give some necessary definitions and results on NETGs. In Section 3, we shall introduce the concepts of ideals and prime ideals on NETGs. We will give the ideal generation formula and consider the set of all ideals on NETGs. In fact, we will prove that the set of all ideals of a NETG, under inclusion order, is a distributive lattice, and construct a NETG on the set of all ideals by endowing it with a special multiplication. In Section 4, we will introduce the topological space (Prim(N),τ) induced by all prime ideals of a NETG N and give necessary and sufficient conditions for the topological space to be a T1-space and a Hausdorff space.
In this section, we will give some concepts and results on NETGs, which will be used in the following sections of this paper.
Definition 1. [11] Let N be a non-empty set together with a binary operation ∗. Then N is called a neutrosophic extended triplet group or NETG for short, if (N,∗) is a semigroup and for any a∈N, there exist a neutral of “a" (denoted by neut(a)) and an opposite of “a" (denoted by anti(a)) such that neut(a)∈N, anti(a)∈N and:
a∗neut(a)=neut(a)∗a=a; |
a∗anti(a)=anti(a)∗a=neut(a). |
Notice that for every element a of a NETG (N,∗), neut(a) is allowed to be equal to the classical identity element of a group, and so all classical groups are special NETGs.
Proposition 1. [16] Let (N,∗) be a NETG. Then for every a∈N, the following statements hold:
(1) neut(a) is unique;
(2) neut(a)∗neut(a)=neut(a);
(3) neut(neut(a))=neut(a).
Notice that anti(a) may be not unique for every element a in a NETG (N,∗), so we use {anti(a)} to denote the set of all opposites of a.
Example 1. Consider Z6={0,1,2,3,4,5} under multiplication ⋅ modulo 6, then (Z6,⋅) is a NETG, in which neut(0)=0, {anti(0)}={0,1,2,3,4,5}; neut(1)=1, {anti(1)}={1}; neut(2)=4, {anti(2)}={2, 5}; neut(3)=3, {anti(3)}={1, 3, 5}; neut(4)=4, {anti(4)}={1, 4}; neut(5)=1, {anti(5)}={5}.
Proposition 2. [20] Let (N,∗) be a NETG. Then the following properties hold: ∀ a∈N, ∀ p, q∈{anti(a)},
(1) p∗neut(a)∈{anti(a)};
(2) p∗neut(a)=q∗neut(a)=neut(a)∗q.
It is well known that in semigroup theory, a−1 is called the inverse element of a and it is unique. Similarly, we can define a unary operation a↦a−1 by a−1=anti(a)∗neut(a) in a NETG (N,∗). Then Proposition 2 indicates that this unary operation is well-defined, and in a NETG (N,∗), a−1∈{anti(a)} and a−1 is determined uniquely for every element a of (N,∗). Moreover, Theorem 2 in [20] declares that in a NETG (N,∗), this unary operation has the following properties:
(a−1)−1=a, a∗a−1∗a=a, a∗a−1=a−1∗a, |
which leads a−1 to be called the inverse element of a in [20]. Therefore, in the following, we will regard a−1 to be anti(a)∗neut(a) for every element a of a NETG (N,∗), and it holds obviously that a−1∗a=a∗a−1=neut(a).
Definition 2. [16] Let (N,∗) be a NETG. If a∗neut(b)=neut(b)∗a for all a, b∈N, then N is called a weak commutative neutrosophic extended triplet group or WCNETG for short.
Proposition 3. [16] Let (N,∗) be a WCNETG. Then for all a, b∈N,
(1) neut(a)∗neut(b)=neut(b∗a);
(2) anti(a)∗anti(b)∈{anti(b∗a)}.
Proposition 4. [21] Let (N,∗) be a NETG, then ∀ a∈N, [neut(a)]−1=neut(a)=neut(a−1).
Proposition 5. [21] Let (N,∗) be a WCNETG, then ∀ a, b∈N, (a∗b)−1=b−1∗a−1.
Definition 3. [16,17] Let (N,∗) is a NETG. A non-empty subset S⊆N is called a NT-subgroup of N if it satisfies the following conditions:
(1) a∗b∈S for all a, b∈S;
(2) {anti(a)}∩S≠∅ for all a∈S.
Example 2. Consider Z6={0,1,2,3,4,5} under multiplication ⋅ modulo 6, from Example 1 we know (Z6,⋅) is a NETG. Then we can list out some NT-subgroups of Z6. For example, S1={0}, S2={1}, S3={3}, S4={4}, S5={0, 1}, S6={0, 3}, S7={0, 4}, S8={2, 4}, S9={1, 3}, S10={1, 5}, S11={0, 2, 4}, S12={0, 2, 3, 4}.
In this section, we are going to propose a special kind of NT-subgroups, called (prime) ideals, of NETGs. Besides presenting the lattice structure of the set of all ideals, we will give the ideal generation formula on NETGs and construct a NETG by endowing the set consisting of all ideals with a special multiplication.
Definition 5. Let (N,∗) be a NETG. A non-empty subset S⊆N is called an ideal of N if for all s∈S and a∈N,
(1) s∗a∈S and a∗s∈S;
(2) {anti(s)}∩S≠∅.
We use Id(N) to denote the set of all ideals on N, then Id(N) is a partially ordered set with the inclusion order ⊆.
Remark 1. (1) From Definition 5 we get that ideals must be NT-subgroups, and every NETG itself is an ideal of its own;
(2) An ideal I is called a proper ideal if I≠N;
(3) For every subset X⊆N, we use ⟨X⟩ to denote the smallest ideal containing X. Hence, if (Id(N),⊆) has the smallest element denoted by I0, then ⟨∅⟩=I0, and we call (N,∗) a NETG with the smallest ideal I0.
Example 3. Refer to Example 1, we can list out all ideals of Z6: I1={0}, I2={0, 2, 4}, I3={0, 3}, I4={0, 2, 3, 4}, I5=Z6.
Example 4. Let N={a, b, c}, and we define multiplication ∗ on N as shown in Table 1.
∗ | a | b | c |
a | a | b | a |
b | b | b | b |
c | a | b | c |
It is easy to verify that (N,∗) is a WCNETG, in which neut(a)=a, {anti(a)}={a, c}, a−1=a; neut(b)=b, {anti(b)}={a, b, c}, b−1=b; neut(c)=c, {anti(c)}={c}, c−1=c.
There are only three ideals of N that are I1={b}, I2={a, b}, I3={a, b, c}.
Proposition 6. Let (N,∗) be a NETG and I an ideal of N. Then for every a∈I, neut(a)∈I and a−1∈I.
Proposition 7. Let (N,∗) be a NETG, then for any subsets I, J∈Id(N), we have I∩J∈Id(N) and I∪J∈Id(N).
Proof. From Proposition 6 it holds obviously.
Corollary 1. Let (N,∗) be a NETG, then (Id(N),∩,∪) is a distributive lattice.
Theorem 1. Let (N,∗) be a WCNETG, then for every non-empty subset X⊆N
⟨X⟩={neut(x)∗y−1:x∈X, y∈N}. |
Proof. Let A={neut(x)∗y−1:x∈X, y∈N}, then for every a∈A, there exist x∈X and y∈N such that a=neut(x)∗y−1. Thus, by Proposition 5, a−1=(neut(x)∗y−1)−1=(y−1)−1∗[neut(x)]−1=(y−1)−1∗neut(x)=neut(x)∗(y−1)−1∈A. Moreover, for every b∈N, a∗b=[neut(x)∗y−1]∗b=neut(x)∗(y−1∗b)=neut(x)∗(b−1∗y)−1∈A, and b∗a=b∗[neut(x)∗y−1]=b∗[y−1∗neut(x)]=(b∗y−1)∗neut(x)=neut(x)∗(y∗b−1)−1∈A. Therefore, A is an ideal. Since for every m∈X, m=neut(m)∗m=neut(m)∗(m−1)−1∈A, we have X⊆A. Let I be an ideal and X⊆I. Then for every n∈A, there exist p∈X and q∈N such that n=neut(p)∗q−1. By Proposition 6 and p∈X⊆I, we have neut(p)∈I, and so n=neut(p)∗q−1∈I. Thus, A⊆I. Hence, ⟨X⟩=A={neut(x)∗y−1:x∈X, y∈N}.
Proposition 8. Let (N,∗) be a WCNETG, then for any a, b∈N, ⟨a⟩∩⟨b⟩=⟨a∗b⟩.
Proof. From Theorem 1 we know ⟨a⟩={neut(a)∗c−1:c∈N}, ⟨b⟩={neut(b)∗d−1:d∈N} and ⟨a∗b⟩={neut(a∗b)∗k−1:k∈N}.
Let x∈⟨a⟩∩⟨b⟩, then there exist c, d∈N such that x=neut(a)∗c−1 and x=neut(b)∗d−1. By Proposition 1 and Proposition 3, we obtain that neut(x)=neut(neut(a)∗c−1)=neut(c−1)∗neut(neut(a))=neut(c−1)∗neut(a). Then by Proposition 4, x=x∗neut(x)=[neut(b)∗d−1]∗[neut(c−1)∗neut(a)]=neut(b)∗[d−1∗(neut(c−1)∗neut(a))]=neut(b)∗[(d−1∗neut(c−1))∗neut(a)]=neut(b)∗[neut(a)∗(d−1∗neut(c−1))]=[neut(b)∗neut(a)]∗[d−1∗neut(c−1)]=neut(a∗b)∗[d−1∗(neut(c))−1]=neut(a∗b)∗[neut(c)∗d]−1∈⟨a∗b⟩. Hence, ⟨a⟩∩⟨b⟩⊆⟨a∗b⟩.
Conversely, let y∈⟨a∗b⟩, then there exist k∈N such that y=neut(a∗b)∗k−1=[neut(b)∗neut(a)]∗k−1=neut(b)∗[neut(a)∗k−1]=neut(b)∗[(neut(a))−1∗k−1] = neut(b)∗[k∗neut(a)]−1∈⟨b⟩. Moreover, y=neut(a∗b)∗k−1=[neut(b)∗neut(a)]∗k−1 = [neut(a)∗neut(b)]∗k−1=neut(a)∗[neut(b)∗k−1]=neut(a)∗[(neut(b))−1∗k−1] = neut(a)∗[k∗neut(b)]−1∈⟨a⟩. Therefore, y∈⟨a⟩∩⟨b⟩, which implies ⟨a∗b⟩⊆⟨a⟩∩⟨b⟩.
Let A and B be two non-empty subsets of N, then we shall use the notation A∗B={a∗b:a∈A, b∈B}.
Theorem 2. Let (N,∗) be a WCNETG. Then for any I1, I2∈Id(N), we have
⟨I1∗I2⟩={a−1∗b−1:a∈I1, b∈I2}. |
Proof. (1) First of all, we will prove that {a−1∗b−1:a∈I1, b∈I2} is an ideal of N.
(i) Let x∈{a−1∗b−1:a∈I1, b∈I2} and y∈N. Then there exist a∈I1 and b∈I2 such that x=a−1∗b−1. Hence, by Proposition 5, x∗y=(a−1∗b−1)∗y=a−1∗(b−1∗y)=a−1∗[(b−1∗y)−1]−1=a−1∗[y−1∗(b−1)−1]−1=a−1∗(y−1∗b)−1. Since I2 is an ideal of N and b∈I2, we have y−1∗b∈I2. Thus, x∗y=a−1∗(y−1∗b)−1∈{a−1∗b−1:a∈I1, b∈I2}. Similarly, we also can prove that y∗x∈{a−1∗b−1:a∈I1, b∈I2}.
(ii) Let z∈{a−1∗b−1:a∈I1, b∈I2}, then there exist c∈I1 and d∈I2 such that z=c−1∗d−1=(d∗c)−1, so by Proposition 4, z−1=[(d∗c)−1]−1=[(d∗c)−1]−1∗neut([(d∗c)−1]−1)=[(d∗c)−1]−1∗[neut((d∗c)−1)]−1. Since I1 is an ideal and c∈I1, we have d∗c∈I1. Then by Proposition 6, we can get (d∗c)−1∈I1. Similarly, since I2 is an ideal and d∈I2, we can get (d∗c)−1∈I2, and then neut((d∗c)−1)∈I2. Therefore, z−1∈{a−1∗b−1:a∈I1, b∈I2}, which means {anti(z)}∩{a−1∗b−1:a∈I1, b∈I2}≠∅.
By (i) and (ii), we conclude that {a−1∗b−1:a∈I1, b∈I2} is an ideal of N.
(2) Next we are going to prove that I1∗I2⊆{a−1∗b−1:a∈I1, b∈I2}. For every x∈I1 and y∈I2, by Proposition 6, x−1∈I1 and y−1∈I2, so x∗y=(x−1)−1∗(y−1)−1∈{a−1∗b−1:a∈I1, b∈I2}.
(3) Let I be an ideal of N and I1∗I2⊆I. For every m∈I1 and n∈I2, by Proposition 6, m−1∈I1 and n−1∈I2, so m−1∗n−1∈I1∗I2⊆I. By arbitrariness of m and n, we have {a−1∗b−1:a∈I1, b∈I2}⊆I, which implies {a−1∗b−1:a∈I1, b∈I2} is the smallest ideal containing I1∗I2. Therefore, ⟨I1∗I2⟩={a−1∗b−1:a∈I1, b∈I2}.
Theorem 3. Let (N,∗) be a WCNETG. If we define a multiplicative operation & on Id(N) by: For all I1, I2∈Id(N),
I1&I2={a−1∗b−1:a∈I1, b∈I2}, |
then (Id(N),&) is a NETG.
Proof. From Theorem 2, we know the multiplicative operation & is well-defined on Id(N).
(1) Firstly, we are going to prove & is associative on Id(N).
Assume that I1, I2 and I3 are three arbitrary ideals of N. Now we will prove (I1&I2)&I3=I1&(I2&I3). By definition of &, we know (I1&I2)&I3={x−1∗y−1:x∈I1&I2, y∈I3}, and I1&(I2&I3)={x−1∗y−1:x∈I1, y∈I2&I3}. For every m∈(I1&I2)&I3, there exist x∈I1&I2 and y∈I3 such that m=x−1∗y−1, and there exist a∈I1 and b∈I2 such that x=a−1∗b−1. Therefore, by Propositions 4 and 5, m=x−1∗y−1=(a−1∗b−1)−1∗y−1=[(b−1)−1∗(a−1)−1]∗y−1=(b∗a)∗y−1=[b∗(neut(a)∗a)]∗y−1=[(b∗neut(a))∗a]∗y−1=[(neut(a)∗b)∗a]∗y−1=neut(a)∗[(b∗a)∗y−1]=(neut(a))−1∗[((b∗a)−1)−1∗y−1]. From Proposition 6 and Remark 3 we can get neut(a)∈I1. Since I2 is an ideal and b∈I2, we have b∗a∈I2, and by Proposition 6 again, (b∗a)−1∈I2. Hence, m=(neut(a))−1∗[((b∗a)−1)−1∗y−1]∈I1&(I2&I3). By arbitrariness of m, we conclude that (I1&I2)&I3⊆I1&(I2&I3). We also can prove I1&(I2&I3)⊆(I1&I2)&I3 in the same way. Consequently, (I1&I2)&I3=I1&(I2&I3). By arbitrariness of I1, I2 and I3, we can conclude that & is associative on Idl(N).
(2) From (1) we know (Id(N),&) is a semigroup. Now we are going to prove (Id(N),&) is a NETG.
Assume that I is an arbitrary ideal of N. It is clear that I&I={a−1∗b−1:a∈I, b∈I}⊆I. Conversely, for every x∈I, since neut(x)∈I and x−1∈I, by Proposition 4, we have x=neut(x)∗x=[neut(x)]−1∗(x−1)−1∈I&I, so by arbitrariness of x, we have I⊆I&I. Therefore, I&I=I, which implies neut(I)=I and I∈{anti(I)}.
By arbitrariness of I, we conclude that (Id(N),&) is a NETG.
Definition 6. Let P be a proper ideal of a NETG (N,∗). Then P is said to be a prime ideal, if for any x, y∈N, x∗y∈P implies x∈P or y∈P.
We use Prim(N) to denote the set of all ideals on N. It is easy to see that I is a prime ideal of the NETG (N,∗) if and only if for all non-empty subsets A, B⊆N, A∗B⊆I implies A⊆I or B⊆I.
Example 5. Refer to Example 1 and Example 3, I2={0, 2, 4}, I3={0, 3} and I4={0, 2, 3, 4} are all prime ideals of the NETG (Z6,⋅). Moreover, in Example 4, I2={a, b} is the unique prime ideal of the NETG (N,∗).
Theorem 4. Let (N,∗) be a WCNETG and I an ideal of N such that x∉I. Then there exists a prime ideal P such that I⊆P and x∉P.
Proof. Assume that I is an ideal and x∉I. Let Π={J∈Id(N)|I⊆J and x∉J}, then I∈Π. From Proposition 6, it is clear that Π satisfies Zorn's Lemma. Let P be a maximal element of Π, then x∉P. Since P≠N, we can choose a, b∈N such that a∉P and b∉P, then P⊆P∪⟨a⟩∈Id(N) and P⊆P∪⟨b⟩∈Id(N). By the maximality of P, we have x∈P∪⟨a⟩ and x∈P∪⟨b⟩. Thus, by Corollary 1 and Proposition 8, we have x∈(P∪⟨a⟩)∩(P∪⟨b⟩)=P∪(⟨a⟩∩⟨b⟩)=P∪⟨a∗b⟩. If a∗b∈P, then P∪⟨a∗b⟩=P, and so x∈P, which is a contradiction. Thus, a∗b∉P, which implies P is a prime ideal.
In this section, we shall define the topological structure on the collection of all prime ideals of a NETG and study some topological properties of the space. Necessary and sufficient conditions will be proposed for the space becoming a T1-space and a Hausdorff space.
Let (N,∗) be a NETG. For A⊆N, we define H(A)={P∈Prim(N)|A⊈P}, and for any a∈N, H(a)=H({a}).
Proposition 9. Let (N,∗) be a NETG. Then for any A, B⊆N, A⊆B implies H(A)⊆H(B).
Proof. If H(A)=∅, then H(A)⊆H(B). If H(A)≠∅, then for every P∈H(A), we have A⊈P, which implies A≠∅ and there exists a∈A such that a∉P. Since A⊆B, we get a∈B, thus, B⊈P, and so P∈H(B). Therefore, H(A)⊆H(B).
Proposition 10. Let (N,∗) be a NETG with the smallest ideal I0. Then for any A, B⊆N, the following statements hold:
(1) H(N)=Prim(N), H(∅)=H(I0)=∅;
(2) if {Ai}i∈Λ is any family of subsets of N, then H(⋃i∈ΛAi)=⋃i∈ΛH(Ai);
(3) H(A)=H(⟨A⟩);
(4) H(A)∩H(B)=H(⟨A⟩∩⟨B⟩).
Proof. (1) It holds obviously.
(2) Since for every i∈Λ, Ai⊆⋃i∈ΛAi, by Proposition 9, we have H(Ai)⊆H(⋃i∈ΛAi) and so ⋃i∈ΛH(Ai)⊆H(⋃i∈ΛAi). Conversely, if H(⋃i∈ΛAi)=∅, then H(⋃i∈ΛAi)⊆⋃i∈ΛH(Ai). If H(⋃i∈ΛAi)≠∅, then for every P∈H(⋃i∈ΛAi), we have ⋃i∈ΛAi⊈P. Thus, there exists i0∈Λ such that Ai0⊈P, and so P∈H(Ai0)⊆⋃i∈ΛH(Ai). Hence, H(⋃i∈ΛAi)⊆⋃i∈ΛH(Ai). Therefore, H(⋃i∈ΛAi)=⋃i∈ΛH(Ai).
(3) Since A⊆⟨A⟩, we have H(A)⊆H(⟨A⟩). Conversely, if H(⟨A⟩)=∅, then H(⟨A⟩)⊆H(A). If H(⟨A⟩)≠∅, then for every P∈H(⟨A⟩), we have ⟨A⟩⊈P. Since A⊆P implies ⟨A⟩⊆P, a contradiction arises. Hence, A⊈P, which means P∈H(A). Thus, H(⟨A⟩)⊆H(A). Therefore, H(A)=H(⟨A⟩).
(4) Applying (3), we only need to prove H(⟨A⟩)∩H(⟨B⟩)=H(⟨A⟩∩⟨B⟩). Since ⟨A⟩∩⟨B⟩⊆⟨A⟩, ⟨B⟩, we have H(⟨A⟩∩⟨B⟩)⊆H(⟨A⟩)∩H(⟨B⟩). Conversely, if H(⟨A⟩)∩H(⟨B⟩)=∅, then H(⟨A⟩)∩H(⟨B⟩)⊆H(⟨A⟩∩⟨B⟩). If H(⟨A⟩)∩H(⟨B⟩)≠∅, then for every P∈H(⟨A⟩)∩H(⟨B⟩), we have ⟨A⟩⊈P and ⟨B⟩⊈P, which implies there exist a∈⟨A⟩ and b∈⟨B⟩ such that a∉P and b∉P. Since P is a prime ideal, we conclude a∗b∉P. However, a∗b∈⟨A⟩∩⟨B⟩. Thus, ⟨A⟩∩⟨B⟩⊈P, that is, P∈H(⟨A⟩∩⟨B⟩). Hence, H(⟨A⟩)∩H(⟨B⟩)⊆H(⟨A⟩∩⟨B⟩). Therefore, H(⟨A⟩)∩H(⟨B⟩)=H(⟨A⟩∩⟨B⟩).
Proposition 11. Let (N,∗) be a NETG. Then for any x, y∈N, the following statements hold:
(1) H(x)∩H(y)=H(x∗y);
(2) ⋃x∈NH(x)=Prim(N);
(3) H(x)=H(neut(x))=H(x−1).
Proof. (1) If H(x∗y)≠∅, then for every P∈H(x∗y), we have x∗y∉P. If x∈P or y∈P, then x∗y∈P, which is a contradiction. Hence, x∉P and y∉P, that is, P∈H(x)∩H(y). Thus, H(x∗y)⊆H(x)∩H(y). Conversely, if H(x)∩H(y)≠∅, then for every P∈H(x)∩H(y), we have x∉P and y∉P. Since P is a prime ideal, we conclude x∗y∉P, that is, P∈H(x∗y). Hence, H(x)∩H(y)⊆H(x∗y). Therefore, H(x)∩H(y)=H(x∗y), and when H(x∗y)=∅ or H(x)∩H(y)=∅, the equation holds obviously.
(2) It follows from Proposition 10 obviously, because N=⋃x∈N{x} and Prim(N)=H(N).
(3) It follows from Proposition 6 obviously.
Let (N,∗) be a NETG with the smallest ideal I0, and let τ={H(X)|X⊆N} be a subset of the power set of Prim(N). Then by Proposition 10, we obtain the following conclusions:
(1) ∅, Prim(N)∈τ;
(2) if H(A), H(B)∈τ, then H(A)∩H(B)∈τ;
(3) if {H(Ai)|i∈Λ}⊆τ, then ⋃i∈ΛH(Ai)∈τ.
Therefore, τ is a topology on Prim(N). We call (Prim(N),τ) a prime ideal space and H(X) an open set in τ.
Proposition 12. Let (N,∗) be a NETG with the smallest ideal I0, then {H(a)|a∈N} is a base of topology (Prim(N),τ).
Proof. For every non-empty subset A⊆N, A=⋃a∈N{a}. From Proposition 10 we get that H(A)=⋃a∈AH(a). Moreover, H(∅)=H(I0).
Proposition 13. Let (N,∗) be a NETG. Then for any I, J∈Id(N), the following hold:
(1) H(I∩J)=H(I)∩H(J);
(2) H(I∪J)=H(I)∪H(J).
Proof. (1) Obviously, H(I∩J)⊆H(I)∩H(J). Conversely, if H(I)∩H(J)=∅, then H(I)∩H(J)⊆H(I∩J). If H(I)∩H(J)≠∅, then for every P∈H(I)∩H(J), I⊈P and J⊈P, which implies there exist a∈I and b∈J such that a∉P and b∉P. Since P is a prime ideal, we have a∗b∉P. However, a∗b∈I∩J, thus, I∩J⊈P, which means P∈H(I∩J). Hence, H(I)∩H(J)⊆H(I∩J). Therefore, H(I∩J)=H(I)∩H(J).
(2) Obviously, H(I)∪H(J)⊆H(I∪J). Conversely, if H(I∪J)=∅, then H(I∪J)⊆H(I)∪H(J). If H(I∪J)≠∅, then for every P∈H(I∪J), we have I∪J⊈P. Since I⊆P and J⊆P imply I∪J⊆P, a contradiction arises. Hence, I⊈P or J⊈P, and so P∈H(I) or P∈H(J), which implies P∈H(I)∪H(J). Thus, H(I∪J)⊆H(I)∪H(J). Therefore, H(I∪J)=H(I)∪H(J).
Theorem 5. Let (N,∗) be a WCNETG with the smallest ideal I0. Then the lattice (Id(N),∩,∪) is isomorphic with the lattice of all open sets in (τ,∩,∪).
Proof. Define a mapping Φ:Id(N)→τ by Φ(I)=H(I) for every I∈Id(N). Let I, J∈Id(N), by Proposition 7 and Proposition 13, we have Φ(I∪J)=H(I∪J)=H(I)∪H(J)=Φ(I)∪Φ(J). Similarly, we get Φ(I∩J)=Φ(I)∩Φ(J). Hence, Φ:Id(N)→τ is a lattice homomorphism. For any H(X)∈τ, by Proposition 10, H(X)=H(⟨X⟩)=Φ(⟨X⟩). Thus, Φ is surjective. On the other hand, let A, B∈Id(N) and Φ(A)=Φ(B), then H(A)=H(B). If A≠B, then there exists a∈A such that a∉B. By Theorem 4, there exists a prime ideal P such that B⊆P and a∉P, which implies A⊈P. Thus, P∈H(A)=H(B). Hence, B⊈P, which is a contradiction. Therefore, A=B, and so Φ is injective.
Theorem 6. Let (N,∗) be a NETG with the smallest ideal I0. Then the following statements are equivalent:
(1) (Prim(N),τ) is a T1-space;
(2) every prime ideal is maximal in (Prim(N),⊆);
(3) every prime ideal is minimal in (Prim(N),⊆).
Proof. (1)⇒(2) Assume that (Prim(N),τ) is a T1-space. Let P∈Prim(N). If there exists a prime ideal Q such that P⊂Q, then there exist subsets A, B⊆X such that P∈H(A) but Q∉H(A), and Q∈H(B) but P∉H(B). Hence, B⊆P⊂Q, and so Q∉H(B), which is a contradiction. Therefore, P is maximal in (Prim(N),⊆).
(2)⇒(3) It holds obviously.
(3)⇒(1) Assume that every prime ideal is minimal in (Prim(N),⊆). Let P, Q be two distinct elements of Prim(N). Since P and Q are minimal in (Prim(N),⊆), we have P⊈Q and Q⊈P, and so there exist a∈P∖Q and b∈Q∖P. Hence, P∈H(b)∖H(a) and Q∈H(a)∖H(b). Therefore, (Prim(N),τ) is a T1-space.
Lemma 1. Let (N,∗) be a NETG. Then for every I, J∈Prim(N), we have I∪J∈Prim(N).
Theorem 7. Let (N,∗) be a NETG with the smallest ideal I0. Then (Prim(N),τ) is a T1-space if and only if (Prim(N),τ) is a Hausdorff-space.
Proof. We only prove necessity. Suppose that (Prim(N),τ) is a T1-space. Let P and Q be two distinct elements of Prim(N). From Theorem 6 we know P and Q are both maximal in (Prim(N),⊆), which implies P⊈Q and Q⊈P, and so there exist a∈P∖Q and b∈Q∖P. Hence, P∈H(b)∖H(a) and Q∈H(a)∖H(b). If H(a)∩H(b)≠∅, then there exists a prime ideal K∈H(a)∩H(b), which means a∉K and b∉K, so P≠K. Since P is maximal in (Prim(N),⊆) and from Lemma 1 we get P⊆P∪K∈Prim(N), we can conclude that P∪K=P must holds. Thus, K⊂P, which is in contradiction with the fact that K is maximal in (Prim(N),⊆). Therefore, H(a)∩H(b)=∅. Hence, (Prim(N),τ) is a Hausdorff-space.
In this paper, inspired by the research work in properties of NT-subgroups in NETGs, we proposed and investigated ideals of NETGs, which are a special kind of NT-subgroups. After studying the lattice structure of (Id(N),⊆), we presented the characterization of the smallest ideal generated by a subset. Moreover, we defined a special multiplication on the set of all ideals of a NETG, which constructed a new NETG. At last, we investigated some topological properties of the prime ideal space. Future research will consider applying fuzzy set theory and rough set theory to the research of algebraic structure of NETGs.
We would like to thank the anonymous referees for the careful reading and valuable comments which have improved the quality of this paper. The research is supported by the National Natural Science Foundation of China (Grant no. 11501435, 11971384) and supported by the PhD research start-up fund (Grant no. BS1529).
The authors declare no conflicts of interest.
[1] | Ortigueira, Fractional calculus for scientists and engineers, New York: Springer, 2011. |
[2] | R. Hilfer, Applications of fractional calculus in physics, Singapore: World Scientific, 2000. |
[3] | R. L. Magin, Fractional calculus in bioengineering, Redding: Begell House, 2006. |
[4] |
Y. M. Lin, C. J. Xu, Finite difference/spectral approximations for the time-fractional diffusion equation, J. Comput. Phys., 225 (2007), 1533–1552. doi: 10.1016/j.jcp.2007.02.001. doi: 10.1016/j.jcp.2007.02.001
![]() |
[5] |
Z. Z. Sun, X. N. Wu, A fully discrete difference scheme for a diffusion-wave system, Appl. Numer. Math., 56 (2006), 193–209. doi: 10.1016/j.apnum.2005.03.003. doi: 10.1016/j.apnum.2005.03.003
![]() |
[6] |
H. F. Ding, C. P. Li, A high-order algorithm for time-Caputo-tempered partial differential equation with Riesz derivatives in two spatial dimensions, J. Sci. Comput., 80 (2019), 81–109. doi: 10.1007/s10915-019-00930-5. doi: 10.1007/s10915-019-00930-5
![]() |
[7] |
Y. Zhao, C. Shen, M. Qu, W. P. Bu, Y. F. Tang, Finite element methods for fractional diffusion equations, Int. J. Model. Simul. Sci. Comput., 11 (2020), 2030001. doi: 10.1142/S1793962320300010. doi: 10.1142/S1793962320300010
![]() |
[8] |
Y. M. Zhao, W. P. Bu, J. F. Huang, D. Y. Liu, Y. F. Tang, Finite element method for two-dimensional space-fractional advection-dispersion equations, Appl. Math. Comput., 257 (2015), 553–565. doi: 10.1016/j.amc.2015.01.016. doi: 10.1016/j.amc.2015.01.016
![]() |
[9] |
H. L. Liao, D. F. Li, J. W. Zhang, Sharp error estimate of the nonuniform L1 formula for linear reaction-subdiffusion equations, SIAM J. Numer. Anal., 56 (2018), 1112–1133. doi: 10.1137/17M1131829. doi: 10.1137/17M1131829
![]() |
[10] |
J. Q. Xie, D. Liang, Z. Y. Zhang, Two novel energy dissipative difference schemes for the strongly coupled nonlinear space fractional wave equations with damping, Appl. Numer. Math., 157 (2020), 178–209. doi: 10.1016/j.apnum.2020.06.002. doi: 10.1016/j.apnum.2020.06.002
![]() |
[11] |
S. B. Yuste, Weighted average finite difference methods for fractional diffusion equations, J. Comput. Phys., 216 (2006), 264–274. doi: 10.1016/j.jcp.2005.12.006. doi: 10.1016/j.jcp.2005.12.006
![]() |
[12] |
Y. Liu, Y. W. Du, H. Li, F. W. Liu, Y. J. Wang, Some second-order θ schemes combined with finite element method for nonlinear fractional cable equation, Numer. Algor., 80 (2019), 533–555. doi: 10.1007/s11075-018-0496-0. doi: 10.1007/s11075-018-0496-0
![]() |
[13] |
L. B. Feng, F. W. Liu, I. Turner, An unstructured mesh control volume method for two-dimensional space fractional diffusion equations with variable coefficients on convex domains, J. Comput. Appl. Math., 364 (2020), 112319. doi: 10.1016/j.cam.2019.06.035. doi: 10.1016/j.cam.2019.06.035
![]() |
[14] |
Y. Liu, Z. D. Yu, H. Li, F. W. Liu, J. F. Wang, Time two-mesh algorithm combined with finite element method for time fractional water wave model, Int. J. Heat Mass Tran., 120 (2018), 1132–1145. doi: 10.1016/j.ijheatmasstransfer.2017.12.118. doi: 10.1016/j.ijheatmasstransfer.2017.12.118
![]() |
[15] |
N. Sene, Analytical solutions and numerical schemes of certain generalized fractional diffusion models, Eur. Phys. J. Plus, 134 (2019), 199. doi: 10.1140/epjp/i2019-12531-4. doi: 10.1140/epjp/i2019-12531-4
![]() |
[16] |
M. Yavuz, N. Sene, Stability analysis and numerical computation of the fractional predator-prey model with the harvesting rate, Fractal Fract., 4 (2020), 35. doi: 10.3390/fractalfract4030035. doi: 10.3390/fractalfract4030035
![]() |
[17] |
G. H. Gao, Z. Z. Sun, H. W. Zhang, A new fractional numerical differentiation formula to approximate the Caputo fractional derivative and its applications, J. Comput. Phys., 259 (2014), 33–50. doi: 10.1016/j.jcp.2013.11.017. doi: 10.1016/j.jcp.2013.11.017
![]() |
[18] |
A. A. Alikhanov, A new difference scheme for the time fractional diffusion equation, J. Comput. Phys., 280 (2015), 424–438. doi: 10.1016/j.jcp.2014.09.031. doi: 10.1016/j.jcp.2014.09.031
![]() |
[19] |
R. Mokhtari, F. Mostajeran, A high order formula to approximate the caputo fractional derivative, Commun. Appl. Math. Comput., 2 (2020), 1–29. doi: 10.1007/s42967-019-00023-y. doi: 10.1007/s42967-019-00023-y
![]() |
[20] |
R. Mokhtari, M. Ramezani, G. Haase, Stability and convergence analyses of the FDM based on some L-type formulae for solving the subdiffusion equation, Numer. Math. Theor. Meth. Appl., 14 (2021), 945–971. doi: 10.4208/nmtma.OA-2021-0020. doi: 10.4208/nmtma.OA-2021-0020
![]() |
[21] |
J. Zhao, Z. C. Fang, H. Li, Y. Liu, A Crank-Nicolson finite volume element method for time fractional Sobolev equations on triangular grids, Mathematics, 8 (2020), 1591. doi: 10.3390/math8091591. doi: 10.3390/math8091591
![]() |
[22] |
J. Zhao, H. Li, Z. C. Fang, Y. Liu, A mixed finite volume element method for time-fractional reaction-diffusion equations on triangular grids, Mathematics, 7 (2019), 600. doi: 10.3390/math7070600. doi: 10.3390/math7070600
![]() |
[23] |
J. Zhao, Z. C. Fang, H. Li, Y. Liu, Finite volume element method with the WSGD formula for nonlinear fractional mobile/immobile transport equations, Adv. Differ. Equ., 2020 (2020), 360. doi: 10.1186/s13662-020-02786-8. doi: 10.1186/s13662-020-02786-8
![]() |
[24] |
J. C. Xu, A novel two-grid method for semilinear elliptic equations, SIAM J. Sci. Comput., 15 (1994), 231–237. doi: 10.1137/0915016. doi: 10.1137/0915016
![]() |
[25] |
J. C. Xu, Two-grid discretization techniques for linear and nonlinear PDEs, SIAM J. Numer. Anal., 33 (1996), 1759–1777. doi: 10.1137/S0036142992232949. doi: 10.1137/S0036142992232949
![]() |
[26] |
C. N. Dawson, M. F. Wheeler, Two-grid methods for mixed finite element approximations of nonlinear parabolic equations, Contemp. Math., 180 (1994), 191–203. doi: 10.1090/conm/180/01971. doi: 10.1090/conm/180/01971
![]() |
[27] |
J. L. Yan, Q. Zhang, L. Zhu, Z. Y. Zhang, Two-grid methods for finite volume element approximations of nonlinear sobolev equations, Numer. Func. Anal. Opt., 37 (2016), 391–414. doi: 10.1080/01630563.2015.1115415. doi: 10.1080/01630563.2015.1115415
![]() |
[28] |
T. L. Hou, L. P. Chen, Y. Yang, Two-grid methods for expanded mixed finite element approximations of semi-linear parabolic integro-differential equations, Appl. Numer. Math., 132 (2018), 163–181. doi: 10.1016/j.apnum.2018.06.001. doi: 10.1016/j.apnum.2018.06.001
![]() |
[29] |
W. Liu, A two-grid method for the semi-linear reaction-diffusion system of the solutes in the groundwater flow by finite volume element, Math. Comput. Simulat., 142 (2017), 34–50. doi: 10.1016/j.matcom.2017.04.004. doi: 10.1016/j.matcom.2017.04.004
![]() |
[30] |
Y. Liu, Y. W. Du, H. Li, J. C. Li, S. He, A two-grid mixed finite element method for a nonlinear fourth-order reaction-diffusion problem with time-fractional derivative, Comput. Math. Appl., 70 (2015), 2474–2492. doi: 10.1016/j.camwa.2015.09.012. doi: 10.1016/j.camwa.2015.09.012
![]() |
[31] |
Y. Liu, Y. W. Du, H. Li, J. F. Wang, A two-grid finite element approximation for a nonlinear time-fractional Cable equation, Nonlinear Dyn., 85 (2016), 2535–-2548. doi: 10.1007/s11071-016-2843-9. doi: 10.1007/s11071-016-2843-9
![]() |
[32] |
Q. F. Li, Y. P. Chen, Y. Q. Huang, Y. Wang, Two-grid methods for semilinear time fractional reaction diffusion equations by expanded mixed finite element method, Appl. Numer. Math., 157 (2020), 38–54. doi: 10.1016/j.apnum.2020.05.024. doi: 10.1016/j.apnum.2020.05.024
![]() |
[33] |
Q. F. Li, Y. P. Chen, Y. Q. Huang, Y. Wang, Two-grid methods for nonlinear time fractional diffusion equations by L1-Galerkin FEM, Math. Comput. Simulat., 185 (2021), 436–451. doi: 10.1016/j.matcom.2020.12.033. doi: 10.1016/j.matcom.2020.12.033
![]() |
[34] |
C. J. Chen, H. Liu, X. C. Zheng, H. Wang, A two-grid MMOC finite element method for nonlinear variable-order time-fractional mobile/immobile advection-diffusion equations, Comput. Math. Appl., 79 (2020), 2771–2783. doi: 10.1016/j.camwa.2019.12.008. doi: 10.1016/j.camwa.2019.12.008
![]() |
[35] |
Y. Liu, N. Liu, H. Li, J. F. Wang, Fast calculation based on a spatial two-grid finite element algorithm for a nonlinear space-time fractional diffusion model, Numer. Meth. Part. D. E., 236 (2020), 1904–1921. doi: 10.1002/num.22509. doi: 10.1002/num.22509
![]() |
[36] | J. E. Jones, A Mixed finite volume element method for accurate computation of fluid velocities in porous media, University of Colorado, Denver, CO, 1995. |
[37] |
S. H. Chou, D. Y. Kwak, P. S. Vassilevski, Mixed covolume methods for the elliptic problems on triangular grids, SIAM J. Numer. Anal., 35 (1998), 1850–1861. doi: 10.1137/S0036142997321285. doi: 10.1137/S0036142997321285
![]() |
[38] |
S. Yang, Z. W. Jiang, Mixed covolume method for parabolic problems on triangular grids, Appl. Math. Comput., 215 (2009), 1251–1265. doi: 10.1016/j.amc.2009.06.068. doi: 10.1016/j.amc.2009.06.068
![]() |
[39] |
H. X. Rui, T. C. Lu, An expanded mixed covolume method for elliptic problems, Numer. Meth. Part. D. E., 21 (2005), 8–23. doi: 10.1002/num.20024. doi: 10.1002/num.20024
![]() |
[40] | Z. C. Fang, J. Zhao, H. Li, Y. Liu, Finite volume element methods for two-dimensional time fractional reaction-diffusion equations on triangular grids, 2021. |
[41] |
D. F. Li, H. L. Liao, W. W. Sun, J. L. Wang, J. W. Zhang, Analysis of L1-Galerkin FEMs for time-fractional nonlinear parabolic problems, Commun. Comput. Phys., 24 (2018), 86–103. doi: 10.4208/cicp.OA-2017-0080. doi: 10.4208/cicp.OA-2017-0080
![]() |
[42] |
F. E. Browder, Existence and uniqueness theorems for solutions of nonlinear boundary value problems, Proc. Symp. Appl. Math., 17 (1965), 24–49. doi: 10.1090/psapm/017/0197933. doi: 10.1090/psapm/017/0197933
![]() |
[43] |
Z. C. Fang, H. Li, An expanded mixed covolume method for sobolev equation with convection term on triangular grids, Numer. Meth. Part. D. E., 29 (2013), 1257–1277. doi: 10.1002/num.21754. doi: 10.1002/num.21754
![]() |
[44] |
J. Douglas, J. E. Roberts, Global estimates for mixed methods for second order elliptic equations, Math. Comput., 44 (1985), 39–52. doi: 10.1090/S0025-5718-1985-0771029-9. doi: 10.1090/S0025-5718-1985-0771029-9
![]() |
[45] |
B. T. Jin, B. Y. Li, Z. Zhou, Correction of high-order BDF convolution quadrature for fractional evolution equations, SIAM J. Sci. Comput., 39 (2017), A3129–A3152. doi: 10.1137/17M1118816. doi: 10.1137/17M1118816
![]() |
[46] |
M. Stynes, E. O'Riordan, J. L. Gracia, Error analysis of a finite difference method on graded meshes for a time-fractional diffusion equation, SIAM J. Numer. Anal., 55 (2017), 1057–1079. doi: 10.1137/16M1082329. doi: 10.1137/16M1082329
![]() |
[47] |
F. H. Zeng, Z. Q. Zhang, G. E. Karniadakis, Second-order numerical methods for multi-term fractional differential equations: Smooth and non-smooth solutions, Comput. Meth. Appl. Mech. Eng., 327 (2017), 478–502. doi: 10.1016/j.cma.2017.08.029. doi: 10.1016/j.cma.2017.08.029
![]() |
[48] |
X. C. Zheng, H. Wang, An optimal-order numerical approximation to variable-order space-fractional diffusion equations on uniform or graded meshes, SIAM J. Numer. Anal., 58 (2020), 330–352. doi: 10.1137/19M1245621. doi: 10.1137/19M1245621
![]() |
[49] |
B. L. Yin, Y. Liu, H. Li, Z. M. Zhang, Finite element methods based on two families of second-order numerical formulas for the fractional Cable model with smooth solutions, J. Sci. Comput., 84 (2020), 2. doi: 10.1007/s10915-020-01258-1. doi: 10.1007/s10915-020-01258-1
![]() |
[50] |
B. L. Yin, Y. Liu, H. Li, Z. M. Zhang, Approximation methods for the distributed order calculus using the convolution quadrature, Discrete Contin. Dyn.-B, 26 (2021), 1447–1468. doi: 10.3934/dcdsb.2020168. doi: 10.3934/dcdsb.2020168
![]() |
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