Abstract
In this article, we are concerned with the existence of weak
1 Introduction
Let
where
We are interested in the existence problem of equation (1.1) when
where
The Hessian equations are important fully nonlinear elliptic equations. They arise naturally from many interesting geometric problems in complex geometry, as illustrated by [8,9,10,17,18,21,22,24,28] and references therein. For the nondegenerate case (i.e.,
When
Based on the above complex Hessian estimate (1.3), Dinew and Kolodziej [6] proved the gradient estimate and got the existence result on a compact Kähler manifold when
For the degenerate case, there are lots of results on degenerate fully nonlinear equations. We first recall some results in the real Euclidean case. Let
When
In this article, we generalize Dinew et al.’s result [7] to the compact Hermitian case with
Theorem 1.1
Let
where we call
By approximation, the above theorem follows from the following a priori estimates.
Theorem 1.2
Let
Then, there exists a uniform constant
Remark 1.3
According to the counterexample by Dinew et al. [7], the assumption
According to the Liouville theorem by Dinew and Kolodziej [6], it is sufficient to prove the
The rest of the article is organized as follows. In Section 2, we prove the Cherrier-type inequality and thus obtain the
2
C
0
-estimate
Lemma 2.1
Let u be a solution of Theorem 1.2. Then, there exists a constant C depending only on
Remark 2.2
Székelyhidi [21] proved the
Motivated by [29], we prove the
We first recall the definition and some inequalities about the
where
Let
Definition 2.3
Let
Similarly, we define
Furthermore,
The following lemma which is similar to Lemma 2.4 in [29] plays an important role during the proof of the Cherrier-type inequality.
Lemma 2.4
There exists a positive constant C depending only on
where
For the
Lemma 2.5
There exist constants
Proof
On the one hand, by equation (1.5), we have
where
where
Multiplying
where we write
Since
where the last inequality follows from Proposition 2.1 in [2]. Thus, we have
To prove the lemma, we want to use term
Direct manipulation gives the following results:
where every
Now, we estimate every term in
From the above equality, we claim that for any
When
where we have used Lemma 2.4 in the last inequality.
By (2.8), we have
Combining the above inequality with (2.5) and (2.6), we obtain
Now, we take
Therefore, we obtain the conclusion
3 Second-order estimate
In this section, we prove the second-order estimate motivated by the auxiliary function in [29], which was first used by [24] on compact Hermitian manifolds. To obtain the second-order estimate depending only on
Lemma 3.1
[7]. Let
Now, we are ready to prove the complex Hessian estimate.
Theorem 3.2
Let u be a solution of Theorem 1.2. Then, there exists a uniform constant C depending only on
Proof
We use the covariant derivative with respect to the Chern connection and denote
We consider the following auxiliary function
where
with
where
Suppose
Similar to [29], we can prove
by choosing
Consider the function
Then,
and
where
For this term
where
Let
We denote by
Then, at
where we use the following Maclaurin’s inequality:
Furthermore,
At the maximum point
First, we can estimate the term
Differentiating the equation
By (3.12) and (3.13), we can estimate
where
where
where we use (3.1) and
Next, we estimate terms
Then, we have
Inserting (3.16) and (3.17) into
where we have used
where we have used
Since
Inserting (3.15), (3.19), and (3.20) into (3.11), we obtain
where
Now, we take
Case 1:
By (3.5), for
Then, we have
where
Substituting (3.22) and (3.23) into (3.21) and by the concavity of
where we use
Inserting (3.9) into (3.24), we obtain
From the above inequality, we have
where
Case 2:
Let
Obviously,
Substituting the above inequality into (3.21), we have
Similar to the proof in [29], we can show that the following four terms on the first line and second lines of (3.28) are nonnegative
We also have
where we assume
Inserting (3.29) and (3.30) into (3.28), we obtain
where we use
By (3.32), we obtain the following estimate:
Finally, combining the estimates (3.26) and (3.31) with (3.33), we obtain the desired estimate as follows:
4 Proof of Theorem 1.1
Since
We next show
To obtain the uniform upper bound of
where in the first inequality we have used the following Maclaurin’s inequality:
Since
Since
Inserting (4.3) and (4.4) into (4.2), we finally obtain the uniform upper bound of
Therefore, we can apply the weak
By taking a subsequence, we obtain the existence of weak
Acknowledgment
The author would like to thank Professor Xinan Ma for his constant support and valuable discussions.
-
Funding information: The research of the author was supported by NSFC 11901102.
-
Conflict of interest: Author states no conflict of interest.
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© 2022 Dekai Zhang, published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
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- Non-degeneracy of bubble solutions for higher order prescribed curvature problem
- On fractional logarithmic Schrödinger equations
- Large solutions of a class of degenerate equations associated with infinity Laplacian
- Chemotaxis-Stokes interaction with very weak diffusion enhancement: Blow-up exclusion via detection of absorption-induced entropy structures involving multiplicative couplings
- Asymptotic mean-value formulas for solutions of general second-order elliptic equations
- Weighted critical exponents of Sobolev-type embeddings for radial functions
- Existence and asymptotic behavior of solitary waves for a weakly coupled Schrödinger system
- On the Lq-reflector problem in ℝn with non-Euclidean norm
- Existence of normalized solutions for the coupled elliptic system with quadratic nonlinearity
- Normalized solutions for a class of scalar field equations involving mixed fractional Laplacians
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- Existence of solutions to contact mean-field games of first order
- The regularity of weak solutions for certain n-dimensional strongly coupled parabolic systems
- Uniform stabilization for a strongly coupled semilinear/linear system
- Existence of nontrivial solutions for critical Kirchhoff-Poisson systems in the Heisenberg group
- Existence of ground state solutions for critical fractional Choquard equations involving periodic magnetic field
- Least energy sign-changing solutions for Schrödinger-Poisson systems with potential well
- Lp Hardy's identities and inequalities for Dunkl operators
- Global well-posedness analysis for the nonlinear extensible beam equations in a class of modified Woinowsky-Krieger models
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