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BY 4.0 license Open Access Published by De Gruyter Open Access July 31, 2019

Monotonicity properties and inequalities related to generalized Grötzsch ring functions

  • Fei Wang , Jian-Hui He , Li Yin and Feng Qi EMAIL logo
From the journal Open Mathematics

Abstract

In the paper, the authors present some monotonicity properties and some sharp inequalities for the generalized Grötzsch ring function and related elementary functions. Consequently, the authors obtain new bounds for solutions of the Ramanujan generalized modular equation.

1 Introduction and main results

For real numbers a, b, and c with c ≠ 0, –1, –2, …, the Gaussian hypergeometric function is defined [1, 4] by

F(a,b;c;x)=2F1(a,b;c;x)=n=0(a)n(b)n(c)nxnn!,|x|<1, (1.1)

where

(x)n=x(x+1)(x+n1),n11,n=0 (1.2)

is called [23] the rising factorial of x ∈ ℂ.

For a, r ∈ (0, 1) and s=1r2, let 𝓚a(r) and 𝓔a(r) denote the generalized elliptic integrals of the first and second kinds which are defined [6] by

Ka=Ka(r)=π2F(a,1a;1;r2)Ka=Ka(r)=Ka(s)Ka(0)=π2Ka(1)= (1.3)

and

Ea=Ea(r)=π2F(a1,1a;1;r2)Ea=Ea(r)=Ea(s)Ea(0)=π2Ea(1)=sin(πa)2(1a) (1.4)

respectively. In the special case a = 12 , the functions 𝓚a(r) and 𝓔a(r) reduce to 𝓚(r) and 𝓔(r) which are the complete elliptic integrals of the first and second kinds [2, 5, 7, 8, 11, 15, 21, 35] respectively. The complete elliptic integrals have many important applications in physics, engineering, geometric function theory, quasi-conformal analysis, theory of mathematical means, number theory, and other fields [6, 8, 9, 10, 17, 31, 32].

In what follows, by the symmetry of (1.3), we assume that a ∈ (0, 12 ].

For real numbers a ∈ (0, 12 ] and r ∈ (0, 1), the generalized Grötzsch ring function μa(r) : (0, 1) → (0, ∞) is defined by

μa(r)=π2sin(πa)Ka(r)Ka(r). (1.5)

In the special case a = 12 , we denote μ1/2(r) by μ(r) which is the modulus of the plane Grötzsch ring B2 ∖ [0, r] for r ∈ (0, 1) and B2 is the unit disk in the plane [3, 6, 24, 28, 36].

It is known that the Ramanujan generalized modular equation with signature 1a of degree p can be expressed by

F(a,1a;1;1s2)F(a,1a;1;s2)=pF(a,1a;1;1r2)F(a,1a;1;r2),0<r<1.

From (1.3) and (1.5), it follows that

μa(s)=pμa(r) (1.6)

and the solution s to the equation (1.6) can be written as

s=φKa(r)=μa1(μa(r)K),K(0,),p=1K.

In the special case a = 12 , the solution φKa (r) reduces to the Hersch–Pfluger distortion function φK(r) which is important in the theory of the plane quasi-conformal mappings. As usual, we call φKa (r) the generalized Hersch–Pfluger distortion function [16, 26, 30, 34].

For real number x > 0, the Euler gamma function Γ and its logarithmic derivative ψ, the so-called digamma or psi function, are defined [1, 19, 20, 22, 29] by

Γ(x)=0tx1etdtandψ(x)=Γ(x)Γ(x)

for ℜ(x) > 0 respectively. For a ∈ (0, 12 ], the so-called Ramanujan constant R(a) is defined [27] by

R(a)=2γψ(a)ψ(1a), (1.7)

where γ is the Euler–Mascheroni constant which can be defined [12, 13, 14, 18] by

limnk=1n(1klnn)=0.5772156649.

By [1, 6.3.4],, we have R ( 12 ) = ln 16.

In 2000, Anderson, Qiu, Vamanamurthy, and Vuorinen discovered relations between bounds of s = φKa (r), μa(r), and ma(r) by establishing in [6, Theorem 6.6] the double inequality

1<exp{(K1)[ma(r)+lnr]}<rKφ1/Ka(r)<exp{(K1)[μa(r)+lnr]} (1.8)

for all r ∈ (0, 1) and K ∈ (1, ∞), where

ma(r)=2πsin(aπ)s2Ka(r)Ka(r)

and ma(r) + ln r is the so-called Hüber function.

During the past decades, the function μa(r) plays an important role in several fields of mathematics. For instance, it is indispensable in the theory of mathematical means, the theory of geometric functions, quasi-conformal theory, and the theory of the Ramanujan modular equations. See [3, 6, 24, 28, 33]. In recent years, convexity and Hölder mean property of the function μa(r) were obtained. Especially, many remarkable properties and sharp inequalities can be found in the literature [3, 33, 36, 37].

The main purpose of this paper is to present some monotonicity properties and some sharp inequalities for the generalized Grötzsch ring function μa(r) and related elementary functions. By applying these results, we establish new bounds for solutions to the Ramanujan generalized modular equation.

Our main results in this paper can be stated as follows.

Theorem 1

For r ∈ (0, 1), a ∈ (0, 12 ], b = 1 – a, and C = R(a)2 , define

F(r)=C[μa(r)+lnr]1(s2artanhr)/r,r(0,1),

where artanh denotes the inverse of the hyperbolic tangent function. Then the function F(r) is strictly increasing from (0, 1) onto (3(a2+b2)4,C). In particular, the double inequality

C(1A1n=1anr2n)<μa(r)+lnr<C(1A2n=1anr2n) (1.9)

holds for A1=1,A2=3(a2+b2)4C,an=24n21, and r ∈ (0, 1).

Theorem 2

For B1=R(a)ln162,B2=B1ln4,B3=3(12a)28,B4=eB1,B5=eB2,B6=B3B1,a(0,12), and r ∈ (0, 1), the following conclusions hold true:

  1. The function

    G1(r)=μa(r)μ(r)s2ln(4/s) (1.10)

    is strictly increasing from (0, 1) onto (B2, ∞). In particular, for r ∈ (0, 1),

    B2s2ln4s<μa(r)μ(r)<B1. (1.11)
  2. The function

    G2(r)=B1[μa(r)μ(r)]1(s2artanhr)/r

    is strictly increasing from (0, 1) onto (B3, B1). In particular, for r ∈ (0, 1),

    B1s2artanhrr<μa(r)μ(r)<B1[1B6(1s2artanhrr)]. (1.12)
  3. Let r0=s,rn=2rn11+rn1=φ2n(s)fornN,A(r)=s2artanhrr,B(r)=s2ln4s,andP(r)=n=0(1+rn)2n. For a ∈ (0, 12 ] and r ∈ (0, 1), we have

    P(r)max{B4A(r),B5B(r)}exp[μa(r)+lnr]P(r)B41B6[1A(r)]. (1.13)

Theorem 3

For C1 = R(a)3ln22ln4 , the function

H(r)=μa(r)artanhss2ln(4/s)

is strictly increasing from (0, 1) onto (C1, ∞). In particular, for r ∈ (0, 1),

C1s2ln4s<μa(r)artanhs<C1ln4. (1.14)

2 Lemmas

For proving our main results, we need the following formulas and lemmas.

The following derivative formulas in [6, Theorem 4.1] and [29] hold true:

dKadr=2(1a)rs2(Eas2Ka),dEadr=2(a1)r(KaEa), (2.1)
ddr(KaEa)=2(1a)rEas2,ddr(Eas2Ka)=2arKa, (2.2)
dμa(r)dr=π24rs2Ka2,KaEa+KaEaKaKa=πsin(aπ)4(1a). (2.3)

Lemma 1

([7, Theorem 1.25]). For –∞ < a < b < ∞, let g, h : [a, b] → ℝ be continuous on [a, b] and differentiable on (a, b) and let h′(x) ≠ 0 on (a, b). If g(x)h(x) is increasing (or decreasing respectively) on (a, b), then so are

g(x)g(a)h(x)h(a)andg(x)g(b)h(x)h(b).

Lemma 2

([2, Lemma 2]). Let rn and sn for n ∈ ℕ be real numbers and the power series

R(x)=n=0r(n)xnandS(x)=n=0s(n)xn

be convergent for |x| < 1. If sn > 0 for n ∈ ℕ and if rnsn is strictly increasing (or decreasing respectively) for n ∈ ℕ, then the function R(x)S(x) is strictly increasing (or decreasing respectively) on (0, 1).

Lemma 3

([6, Lemmas 5.2 and 5.4] and [25, Theorem 2.2]). For r ∈ (0, 1) and b = 1 – a, the following conclusions hold true:

  1. the function Eas2Kar2 is strictly increasing from (0, 1) onto (aπ2,sin(aπ)2b) ;

  2. the function KaEaln(1/s) is strictly decreasing from (0, 1) onto (sin(), (1 – a)π);

  3. the function π2/4s2Ka2r2 is strictly increasing from (0, 1) onto ((a2+b2)π24,π24) ;

  4. the function sc𝓚a is decreasing from (0, 1) onto (0, π2 ) if and only if c ≥ 2a(1 – a); the function s 𝓚a(r) is decreasing for each a ∈ (0, 12 ];

  5. the function E1s2ln(4/s) is strictly increasing from (0, 1) onto (π22ln4,12).

Lemma 4

([6, Theorem 5.5] and [24, Theorems 1 and 2]). Let R(a) be the Ramanujan constant defined in (1.7). Then

  1. the function μa(r) + ln r is strictly decreasing from (0, 1) onto (0, R(a)2 );

  2. the function μa(r) – μ(r) is strictly decreasing from (0, 1) onto (0,R(a)ln162) ;

  3. the function μa(r) – artanh s is strictly decreasing from (0, 1) onto the interval (0,R(a)3ln22).

Lemma 5

For r ∈ (0, 1) and b = 1 – a, the following conclusions hold true:

  1. the function

    I1(r)=ln(1/s)(1+r2)(artanhr)/r1

    is strictly increasing from (0, 1) onto (38,12) ;

  2. the function

    I2(r)=KaEa(12a)(Eas2Ka)r2

    is strictly increasing from (0, 1) onto ((a2+b2)π2,) ;

  3. the function

    I3(r)=π2/(4s2Ka2)1ln(1/s)

    is strictly increasing from (0, 1) onto (2(a2 + b2), ∞).

Proof

Utilizing (1.1) and [29, 2.2.5] and using power series expansion lead to

ln1s=n=0r2n+22(n+1) (2.4)

and

artanhr=rF(12,1;32;r2)=n=0r2n+12n+1. (2.5)

Applying (2.5) yields

(1+r2)artanhrr1=n=012n+1r2n+n=012n+1r2n+21=n=0(12n+1+12n+3)r2n+2=n=04(n+1)(2n+1)(2n+3)r2n+2,

from which and (2.4), it follows that

I1(r)=ln(1/s)(1+r2)(artanhr)/r1=n=0a1(n)r2nn=0b1(n)r2n,

where

a1(n)=12(n+1)andb1(n)=4(n+1)(2n+1)(2n+3).

Let c1(n)=a1(n)b1(n). Then

c1(n)c1(n+1)=(2n+1)(n+2)2(2n+5)(n+1)2<1. (2.6)

Hence, the inequality (2.6) implies that c1(n) is strictly increasing in n. From Lemma 2, it follows that I1(r) is strictly increasing in (0, 1).

By virtue of L’Hôpital’s rule and Lemma 5, we easily obtain the limits I1(0+)=38andI1(1)=12.

From (1.1) to (1.4), it is easy to verify that

KaEa=π2n=0(a)n(1a)n+1(n+1)(n!)2r2n+2

and

Eas2Ka=aπ2n=0(a)n(1a)n(n+1)(n!)2r2n+2

for r ∈ (0, 1). Hence, after simplifying and utilizing (1.2), the function I2(r) can be rewritten as

I2(r)=π2[n=0(a)n(1a)n+1(n+1)(n!)2r2na(12a)n=0(a)n(1a)n(n+1)(n!)2r2n]=π2n=0Jn(n+1)(n!)2r2n,

where Jn = [a2 + b2 + n](a)n(1 – a)n and b = 1 – a. A conclusion in [6, Lemma 7.1] states that the function (x)n+1(1 – x)n+1 for n ≥ 0 is positive, increasing on [0, 12 ], and decreasing on [ 12 , 1]. This implies that Jn > 0. Thus, the monotonicity of I2(r) follows immediately.

The limits limx0+I2(x)=(a2+b2)π2 and limx→1 I2(x) = ∞ are straightforward.

Let I3(r)=I4(r)I5(r), where I4(r)=π24s2Ka21 and I5(r)=ln1s. By (1.3), it follows that limx→0+ I4(x) = limx→0+ I5(x) = 0.

From the formula (2.1) and elementary computation, it follows that

I4(r)I5(r)=π221s4Ka3r2Ka2(1a)(Eas2Ka)rs2r=π221s2Ka3KaEa(12a)(Eas2Ka)r2.

From Lemma 1, the fourth item in Lemma 3, and the second item in Lemma 5, the monotonicity of I3(r) follows immediately.

By L’Hôpital’s rule and Lemmas 3 and 5, we arrive at

limr0+I3(r)=limr0+I4(r)I5(r)=π221(π/2)3(a2+b2)π2=2(a2+b2),

while limr→1 I3(r) = ∞ directly. The proof of Lemma 5 is complete.□

Lemma 6

For r ∈ (0, 1) and b = 1 – a, we have the following conclusions:

  1. the function L1(r)=KKaln(1/s) is strictly increasing from (0, 1) onto the interval (π(12a)24,1sin(aπ)) ;

  2. the function L2(r)=KKaKaEa is strictly increasing from (0, 1) onto the interval ((12a)24b,1sin(aπ)1) ; the function KKaKE is strictly increasing from (0, 1) onto ((12a)22,1sin(aπ)) ;

  3. the function L3(r)=KKa(1+r2)(artanhr)/r1 is strictly increasing from (0, 1) onto (3π(12a)232,1sin(aπ)2).

Proof

Let 1(r) = 𝓚 – 𝓚a and 2(r) = ln 1s . It is obvious that L1(r)=1(r)2(r) and limr→0+1(r) = limr→0+ 2(r) = 0.

It follows from (1.3) and (2.1) that

1(r)2(r)=Es2K2(1a)(Eas2Ka)r2=3(r)4(r),

where

3(r)=Es2K2(1a)(Eas2Ka)and4(r)=r2.

It is clear that limr→0+ 3(r) = limr→0+ 4(r) = 0. Applying (2.2) and (1.3) and differentiating give

3(r)4(r)=K4a(1a)Ka2=π4n=0Tn(n!)2r2n,

where Tn=(12)n(12)n4a(1a)(a)n(1a)n. From [6, Lemma 7.1], it is easy to see that Tn ≥ 0. Therefore, the monotonicity of L1(r) follows from Lemma 2.

By L’Hôpital’s rule and Lemmas 1 and 3, we have

limr0+L1(r)=limr0+1(r)2(r)=limr0+3(r)4(r)=π(12a)24.

It is known [4, (1.6)] that F(a, b; a + b; x) satisfies the Ramanujan asymptotic relation

B(a,b)F(a,b;a+b;x)+ln(1x)=R(a,b)+O((1x)ln(1x)),x1

for a, b ∈ (0, ∞), where R(a, b) = –2γψ(a) – ψ(b) and

limx1F(a,1a;1;x)ln[1/(1x)]=1B(a,1a), (2.7)

where

B(a,1a)=Γ(a)Γ(1a)=πsin(aπ). (2.8)

Hence, the limit limr→1 L1(r) = 1 – sin() follows from (1.3), (2.7), and (2.8).

The function L2(r) can be rewritten as

L2(r)=KKaln(1/s)ln(1/s)KaEa.

Hence, the monotonicity property of the function L2(r) follows from the second item in Lemma 3 and the first item in 6. Furthermore, the limits

limr0+L2(r)=(12a)24(1a)andlimr1L2(r)=1sinaπ1

are easily obtained. Similarly, we can prove that the function KKaKE is strictly increasing from (0, 1) onto ((12a)22,1sin(aπ)).

The function L3(r) can be rewritten as

L3(r)=KKaln(1/s)ln(1/s)(1+r2)(artanhr)/r1.

From the first items in Lemmas 5 and 6, the monotonicity of L3(r) follows immediately. Moreover, the limits

limr0+L3(r)=3π(12a)232andlimr1L3(r)=1sin(aπ)2

can be obtained from the first items in Lemmas 5 and 6. The proof of Lemma 6 is complete.□

3 Proofs of main results

Now we are in a position to prove our main results.

Proof of Theorem 1

Let

f1(r)=C[μa(r)+lnr]andf2(r)=1s2artanhrr.

Then F(r)=f1(r)f2(r) and, by Lemma 4, f1(0+) = f2(0+) = 0.

Differentiating and making use of (2.3) give

f1(r)f2(r)=π2/(4s2Ka2)1(1+r2)(artanhr)/r1=π2/(4s2Ka2)1ln(1/s)ln(1/s)(1+r2)(artanhr)/r1.

From Lemmas 1 and the first and third conclusions in Lemma 5, we see that the function F(r) is strictly increasing on (0, 1).

By L’Hôpital’s rule and the first and third items in Lemma 5, we obtain

limr0F(r)=limr0f1(r)f2(r)=3(a2+b2)4.

Clearly, the limit F(1) = R(a)2 follows from the first item in Lemma 4.

Finally, by (2.5), the double inequality in (1.9) follows from the monotonicity property of F(r). The proof of Theorem 1 is complete.□

Corollary 1

For r ∈ (0, 1) and K ∈ (1, ∞), the inequality

φ1/Ka(r)>rKexp{C(1K)[1n=1anr2n]} (3.1)

holds true, where C=R(a)2andan=24n21.

Proof

This follows from combining (1.8) with the double inequality (1.9).□

Remark 1

The upper and lower bounds in (1.9) are better than corresponding bounds in

C[1abπsin(aπ)n=0anr2n+2]<μa(r)+lnr<C[1a2+b22cn=0anr2n+2]

obtained in [34, Theorem 2].

The inequality (3.1) gives an elementary and infinite series estimates for φ1/Ka (r) and, consequently, the bound of solutions to the Ramanujan generalized modular equations is refined.

Proof of Theorem 2

Write G1(r) as

G1(r)=μa(r)μ(r)E1E1s2ln(4/s)=g1(r)g2(r),

where

g1(r)=μa(r)μ(r)E1andg2(r)=E1s2ln(4/s).

Let g3(r) = μa(r) – μ(r) and g4(r) = 𝓔 – 1. By (1.4) and the second item in Lemma 4, we obtain

g1(r)=g3(r)g4(r)andg3(1)=g4(1)=0.

Direct computation and utilization of (2.1) and (2.3) result in

g3(r)g4(r)=π24K+KasK2sKa2KKaKE. (3.2)

Hence, from the fourth item in Lemma 3 and the second item in Lemma 6, it follows that the function g1(r) is strictly increasing on (0, 1). Using L’Hôpital’s rule together with the fifth item in Lemma 3 and the second item in Lemma 6, the limits g1(0)=R(a)ln16π2 and g1(1) = ∞ follows readily.

By (3.2), the function G1(r) is a product of two positive and strictly increasing functions, so the monotonicity of G1(r) follows from the fifth item in Lemma 3. From the fifth item in Lemma 3 and the limit of g1(r), we gain G1(0+)=R(a)ln162ln4 and G1(1) = ∞. Moreover, the double inequality (1.11) is obvious.

Let g5(r) = B1 – [μa(r) – μ(r)] and g6(r)=1s2artanhrr. Then G2(r)=g5(r)g6(r) and g5(0) = g6(0) = 0. By (2.3), simple computation leads to

g5(r)g6(r)=π24K2Ka2s2K2Ka21(1+r2)(artanhr)/r1=π24K+Ka(sK2)(sKa2)KKa(1+r2)(artanhr)/r1.

Hence, by Lemma 1, the monotonicity of G2(r) follows from the fourth item in Lemma 3 and the third item in Lemma 6.

Clearly, the limit G2(1)=R(a)ln162 is valid. By L’Hôpital’s rule and the third item in Lemma 6, we readily obtain

limr0G2(r)=limr0g5(r)g6(r)=3(12a)28.

By the monotonicity of G2(r), the double inequality (1.12) follows immediately.

By the formula (1.11) in [28, Theorem 1], we have

exp(μ(r)+lnr)=n=0(1+rn)2n=P(r). (3.3)

Consequently, the third item in Theorem 2 follows from (1.11) and (1.12). The proof of Theorem 2 is complete.□

Corollary 2

For r ∈ (0, 1) and K ∈ (1, ∞), the inequality

φ1/Ka(r)>[max{B4A(r),B5B(r)}n=0(1+rn)1/2n]rKeK (3.4)

holds true, where A(r)=s2artanhrrandB(r)=s2ln4s.

Proof

This follows from combining the double inequality (1.8), the equality (3.3), and the inequality (1.13).□

Remark 2

The lower bound in (1.11) is better than the corresponding bound in the equation (11) in [24, Theorem 1] which is referenced in item (2) of Lemma 4.

The upper and lower bounds in (1.12) are better than corresponding bounds in the equation (11) in [24, Theorem 1] which is referenced in item (2) of Lemma 4.

The inequality (3.4) provides an elementary and an infinite product estimates for φ1/Ka (r) and a new bound of solutions to the Ramanujan generalized modular equations is given.

Proof of Theorem 3

It is easy to see that the function H(r) can be written as

H(r)=μa(r)μ(r)s2ln(4/s)+μ(r)artanhss2ln(4/s)=G1(r)+H1(r), (3.5)

where G1(r) is defined by (1.10) and

H1(r)=μ(r)artanhss2ln(4/s) (3.6)

which can be equivalently written as the product of two functions

H1(r)=μ(r)artanhsE1E(r)1s2ln(4/s). (3.7)

Denote

h1(r)=μ(r)artanhsE1=h2(r)h3(r),

where h2(r) = μ(r) – artanh s and h3(r) = 𝓔 – 1. By the third item in Lemma 4 and (1.4), we obtain h2(1) = h3(1) = 0. Applying (2.1) and (2.3) and simply computing yield

h2(r)h3(r)=12π22s(1+s)K2s2K2(KE)=12π22s(1+s)K2r21sK2(r)r2s(KE).

Let

h4(r)=π22s(1+s)K2(r)r2 (3.8)

and s=1r2. Using the substitution

r=2u1+uandu=2t1+t. (3.9)

Then u=1t1+t. By Landen’s transformation formula

K(2r1+r)=(1+r)K(r)

in [30] and (3.9), we have

K(r)=(1+u)K(u)=(1+u)(1+t)K(t). (3.10)

By (3.10), the identity (3.8) is equivalent to

h4(r)=(t+t)44(1+t)t(π/2)2[tK(t)]2t2. (3.11)

It is easy to show that the first factor in the right hand side of (3.11) is strictly increasing in t on (0, 1). Hence, by virtue of the third item in Lemma 3 and the relation between r and t, the function h4(r) is strictly increasing on (0, 1).

It was given in [2, Theorem 15] that the function rs(KE)r2 is strictly decreasing from (0, 1) onto (0,π4). Therefore, by (3.7) and Lemma 1, the function h1(r) is positive and strictly increasing.

From the fifth item in Lemma 3 and (3.6), we conclude that the function H1(r) is strictly increasing on (0, 1). Hence, the monotonicity of H(r) follows from the first item in Theorem 2 and (3.5).

It is clear that the limits H1(0+) = 14 and H1(1) = ∞ follow from item (5) in Lemma 3, item (1) in Lemma 4, and item (1) in Theorem 2. Additionally we note that H(0+) = G1(o+) + H1(o+) = R(a)ln162ln4 . The double inequality (1.14) follows immediately. The proof of Theorem 3 is complete.□

Remark 3

The lower bound in (1.14) is better than corresponding bounds in the equation (14) in [24, Theorem 2] which is presented in item (3) of Lemma 4.


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Acknowledgements

This research was partially supported by the Natural Science Foundation of China (Grant No. 11171307 and 11401041), the Natural Science Foundation of the Educational Department of Zhejiang (Grant No. Y201635387 and Y201840023), the Science and Technology Foundation of Shandong (Grant No. J16li52), and Zhejiang Higher Education Visiting Scholar Foundation (Grant No. FX2018093).

The authors appreciate anonymous referees for their careful corrections and valuable comments on the original version of this paper.

  1. Authors’ Contributions: All authors contributed equally to the manuscript and read and approved the final manuscript.

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Received: 2018-08-21
Accepted: 2019-05-29
Published Online: 2019-07-31

© 2019 Wang et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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