Datasets:
record_id string | paper_system_number int64 | task_type string | problem_name string | tier string | dimension int64 | time_domain string | dynamics string | specification_latex string | citations list | problem_json string | executable_record_json string | descriptive_record_json string |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
DCB-LIT-P1-001 | 1 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -((1)/(2))*tan(((pi*x1)/(2))+((pi)/(4)))+x2+((1)/(2)), dx2/dt = x1-((1)/(2))*tan(((pi*x2)/(2))+((pi)/(4)))+((1)/(2)) | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -\dfrac{1}{2}\tan\left(\dfrac{\pi x_1}{2} + \dfrac{\pi}{4}\right) + x_2 + \dfrac{1}{2}\\[1.5ex] x_1 - \dfrac{1}{2}\tan\left(\dfrac{\pi x_2}{2} + \dfrac{\pi}{4}\right) + \dfrac{1}{2} \end{pmatrix}. \] | [
"khalil2002nonlinear"
] | {"problem_id":"dcb_lit_p1_001","task_type":"stability","name":"DynaCertBench System 001 · DCB-LIT-P1-001 · Exercise~4.30, \\cite{khalil2002nonlinear}","dynamics":"dx1/dt = -((1)/(2))*tan(((pi*x1)/(2))+((pi)/(4)))+x2+((1)/(2)), dx2/dt = x1-((1)/(2))*tan(((pi*x2)/(2))+((pi)/(4)))+((1)/(2))","source":"paper System 1; cano... | {"record_id":"DCB-LIT-P1-001","problem":{"problem_id":"dcb_lit_p1_001","task_type":"stability","name":"DynaCertBench System 001 · DCB-LIT-P1-001 · Exercise~4.30, \\cite{khalil2002nonlinear}","dynamics":"dx1/dt = -((1)/(2))*tan(((pi*x1)/(2))+((pi)/(4)))+x2+((1)/(2)), dx2/dt = x1-((1)/(2))*tan(((pi*x2)/(2))+((pi)/(4)))+(... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-002 | 2 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -x1+x1*x2, dx2/dt = -x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_1+x_1x_2\\ -x_2 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_002","task_type":"stability","name":"DynaCertBench System 002 · DCB-LIT-P1-002 · Table~1 row~1 (NonPoly0), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1+x1*x2, dx2/dt = -x2","source":"paper System 2; canonical record DCB-LIT-P1-002","assumptions":["Deterministically normalized from canonic... | {"record_id":"DCB-LIT-P1-002","problem":{"problem_id":"dcb_lit_p1_002","task_type":"stability","name":"DynaCertBench System 002 · DCB-LIT-P1-002 · Table~1 row~1 (NonPoly0), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1+x1*x2, dx2/dt = -x2","source":"paper System 2; canonical record DCB-LIT-P1-002","assumptions":["D... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-003 | 3 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -x1+2*x1**2*x2, dx2/dt = -x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_1+2x_1^2x_2\\ -x_2 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_003","task_type":"stability","name":"DynaCertBench System 003 · DCB-LIT-P1-003 · Table~1 row~2 (NonPoly1), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1+2*x1**2*x2, dx2/dt = -x2","source":"paper System 3; canonical record DCB-LIT-P1-003","assumptions":["Deterministically normalized from ca... | {"record_id":"DCB-LIT-P1-003","problem":{"problem_id":"dcb_lit_p1_003","task_type":"stability","name":"DynaCertBench System 003 · DCB-LIT-P1-003 · Table~1 row~2 (NonPoly1), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1+2*x1**2*x2, dx2/dt = -x2","source":"paper System 3; canonical record DCB-LIT-P1-003","assumptions... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-004 | 4 | stability | Stability certification | literature | 3 | continuous | dx1/dt = -x1, dx2/dt = -2*x2+0.1*x1*x2**2+x3, dx3/dt = -x3-1.5*x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -x_1\\ -2x_2+0.1x_1x_2^2+x_3\\ -x_3-1.5x_2 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_004","task_type":"stability","name":"DynaCertBench System 004 · DCB-LIT-P1-004 · Table~1 row~3 (NonPoly2), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1, dx2/dt = -2*x2+0.1*x1*x2**2+x3, dx3/dt = -x3-1.5*x2","source":"paper System 4; canonical record DCB-LIT-P1-004","assumptions":["Determin... | {"record_id":"DCB-LIT-P1-004","problem":{"problem_id":"dcb_lit_p1_004","task_type":"stability","name":"DynaCertBench System 004 · DCB-LIT-P1-004 · Table~1 row~3 (NonPoly2), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1, dx2/dt = -2*x2+0.1*x1*x2**2+x3, dx3/dt = -x3-1.5*x2","source":"paper System 4; canonical record ... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\... |
DCB-LIT-P1-005 | 5 | stability | Stability certification | literature | 3 | continuous | dx1/dt = -3*x1-0.1*x1*x2**3, dx2/dt = -x2+x3, dx3/dt = -x3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -3x_1-0.1x_1x_2^3\\ -x_2+x_3\\ -x_3 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_005","task_type":"stability","name":"DynaCertBench System 005 · DCB-LIT-P1-005 · Table~1 row~4 (NonPoly3), \\cite{abate2021fossil}","dynamics":"dx1/dt = -3*x1-0.1*x1*x2**3, dx2/dt = -x2+x3, dx3/dt = -x3","source":"paper System 5; canonical record DCB-LIT-P1-005","assumptions":["Deterministical... | {"record_id":"DCB-LIT-P1-005","problem":{"problem_id":"dcb_lit_p1_005","task_type":"stability","name":"DynaCertBench System 005 · DCB-LIT-P1-005 · Table~1 row~4 (NonPoly3), \\cite{abate2021fossil}","dynamics":"dx1/dt = -3*x1-0.1*x1*x2**3, dx2/dt = -x2+x3, dx3/dt = -x3","source":"paper System 5; canonical record DCB-LIT... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\... |
DCB-LIT-P1-006 | 6 | stability | Stability certification | literature | 3 | continuous | dx1/dt = -x1**3-x1*x3**2, dx2/dt = -x2-x1**2*x2, dx3/dt = -x3+3*x1**2*x3-3*x3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -x_1^3-x_1x_3^2\\ -x_2-x_1^2x_2\\ -x_3+3x_1^2x_3-3x_3 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_006","task_type":"stability","name":"DynaCertBench System 006 · DCB-LIT-P1-006 · Table~1 row~5 (Poly1), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3-x1*x3**2, dx2/dt = -x2-x1**2*x2, dx3/dt = -x3+3*x1**2*x3-3*x3","source":"paper System 6; canonical record DCB-LIT-P1-006","assumptions":[... | {"record_id":"DCB-LIT-P1-006","problem":{"problem_id":"dcb_lit_p1_006","task_type":"stability","name":"DynaCertBench System 006 · DCB-LIT-P1-006 · Table~1 row~5 (Poly1), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3-x1*x3**2, dx2/dt = -x2-x1**2*x2, dx3/dt = -x3+3*x1**2*x3-3*x3","source":"paper System 6; canonica... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\... |
DCB-LIT-P1-007 | 7 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -x1**3+x2, dx2/dt = -x1-x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_1^3+x_2\\ -x_1-x_2 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_007","task_type":"stability","name":"DynaCertBench System 007 · DCB-LIT-P1-007 · Table~1 row~6 (Poly2), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3+x2, dx2/dt = -x1-x2","source":"paper System 7; canonical record DCB-LIT-P1-007","assumptions":["Deterministically normalized from canonic... | {"record_id":"DCB-LIT-P1-007","problem":{"problem_id":"dcb_lit_p1_007","task_type":"stability","name":"DynaCertBench System 007 · DCB-LIT-P1-007 · Table~1 row~6 (Poly2), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3+x2, dx2/dt = -x1-x2","source":"paper System 7; canonical record DCB-LIT-P1-007","assumptions":["D... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-008 | 8 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -x1**3-x2**2, dx2/dt = x1*x2-x2**3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_1^3-x_2^2\\ x_1x_2-x_2^3 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_008","task_type":"stability","name":"DynaCertBench System 008 · DCB-LIT-P1-008 · Table~1 row~7 (Poly3), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3-x2**2, dx2/dt = x1*x2-x2**3","source":"paper System 8; canonical record DCB-LIT-P1-008","assumptions":["Deterministically normalized from... | {"record_id":"DCB-LIT-P1-008","problem":{"problem_id":"dcb_lit_p1_008","task_type":"stability","name":"DynaCertBench System 008 · DCB-LIT-P1-008 · Table~1 row~7 (Poly3), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1**3-x2**2, dx2/dt = x1*x2-x2**3","source":"paper System 8; canonical record DCB-LIT-P1-008","assumpti... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-009 | 9 | stability | Stability certification | literature | 2 | continuous | dx1/dt = -x1-1.5*x1**2*x2**3, dx2/dt = -x2**3+0.5*x1**3*x2**2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_1-1.5x_1^2x_2^3\\ -x_2^3+0.5x_1^3x_2^2 \end{pmatrix}. \] | [
"abate2021fossil"
] | {"problem_id":"dcb_lit_p1_009","task_type":"stability","name":"DynaCertBench System 009 · DCB-LIT-P1-009 · Table~1 row~8 (Poly4), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1-1.5*x1**2*x2**3, dx2/dt = -x2**3+0.5*x1**3*x2**2","source":"paper System 9; canonical record DCB-LIT-P1-009","assumptions":["Deterministical... | {"record_id":"DCB-LIT-P1-009","problem":{"problem_id":"dcb_lit_p1_009","task_type":"stability","name":"DynaCertBench System 009 · DCB-LIT-P1-009 · Table~1 row~8 (Poly4), \\cite{abate2021fossil}","dynamics":"dx1/dt = -x1-1.5*x1**2*x2**3, dx2/dt = -x2**3+0.5*x1**3*x2**2","source":"paper System 9; canonical record DCB-LIT... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-010 | 10 | stability | Stability certification | literature | 2 | continuous | dx1/dt = x2+u1, dx2/dt = u2+((3/20)*(981/100)*(1/2)*sin(x1)-(1/10)*x2)/((3/20)*(1/2)**2) | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} x_2+u_1\\ u_2+\dfrac{mgL\sin(x_1)-bx_2}{mL^2} \end{pmatrix}, \] where $m=0.15$, $g=9.81$, $L=0.5$, and $b=0.1$. | [
"edwards2024fossil"
] | {"problem_id":"dcb_lit_p1_010","task_type":"stability","name":"DynaCertBench System 010 · DCB-LIT-P1-010 · Table~4 \\#2 (SineModel), \\cite{edwards2024fossil}","dynamics":"dx1/dt = x2+u1, dx2/dt = u2+((3/20)*(981/100)*(1/2)*sin(x1)-(1/10)*x2)/((3/20)*(1/2)**2)","source":"paper System 10; canonical record DCB-LIT-P1-010... | {"record_id":"DCB-LIT-P1-010","problem":{"problem_id":"dcb_lit_p1_010","task_type":"stability","name":"DynaCertBench System 010 · DCB-LIT-P1-010 · Table~4 \\#2 (SineModel), \\cite{edwards2024fossil}","dynamics":"dx1/dt = x2+u1, dx2/dt = u2+((3/20)*(981/100)*(1/2)*sin(x1)-(1/10)*x2)/((3/20)*(1/2)**2)","source":"paper Sy... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-011 | 11 | stability | Stability certification | literature | 2 | discrete | x1[k+1] = 0.687*x1+0.558*x2-0.0001*x1*x2, x2[k+1] = -0.292*x1+0.773*x2 | The discrete-time transition map is: \[ \mathbf{x}^{+} = F(\mathbf{x}) = \begin{pmatrix} 0.687x_1+0.558x_2-0.0001x_1x_2\\ -0.292x_1+0.773x_2 \end{pmatrix}. \] | [
"edwards2024fossil"
] | {"problem_id":"dcb_lit_p1_011","task_type":"stability","name":"DynaCertBench System 011 · DCB-LIT-P1-011 · Table~4 \\#14 (DTAhmadi2), \\cite{edwards2024fossil}","dynamics":"x1[k+1] = 0.687*x1+0.558*x2-0.0001*x1*x2, x2[k+1] = -0.292*x1+0.773*x2","source":"paper System 11; canonical record DCB-LIT-P1-011","assumptions":[... | {"record_id":"DCB-LIT-P1-011","problem":{"problem_id":"dcb_lit_p1_011","task_type":"stability","name":"DynaCertBench System 011 · DCB-LIT-P1-011 · Table~4 \\#14 (DTAhmadi2), \\cite{edwards2024fossil}","dynamics":"x1[k+1] = 0.687*x1+0.558*x2-0.0001*x1*x2, x2[k+1] = -0.292*x1+0.773*x2","source":"paper System 11; canonica... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-012 | 12 | stability | Stability certification | literature | 2 | discrete | x1[k+1] = 0.3*x1+u1, x2[k+1] = -x1+0.5*x2+((7)/(18))*x1**2+u2 | The discrete-time transition map is: \[ \mathbf{x}^{+} = F(\mathbf{x},\mathbf{u}) = \begin{pmatrix} 0.3x_1+u_1\\ -x_1+0.5x_2+\dfrac{7}{18}x_1^2+u_2 \end{pmatrix}. \] | [
"edwards2024fossil"
] | {"problem_id":"dcb_lit_p1_012","task_type":"stability","name":"DynaCertBench System 012 · DCB-LIT-P1-012 · Table~4 \\#15 (DTAhmadi), \\cite{edwards2024fossil}","dynamics":"x1[k+1] = 0.3*x1+u1, x2[k+1] = -x1+0.5*x2+((7)/(18))*x1**2+u2","source":"paper System 12; canonical record DCB-LIT-P1-012","assumptions":["Determini... | {"record_id":"DCB-LIT-P1-012","problem":{"problem_id":"dcb_lit_p1_012","task_type":"stability","name":"DynaCertBench System 012 · DCB-LIT-P1-012 · Table~4 \\#15 (DTAhmadi), \\cite{edwards2024fossil}","dynamics":"x1[k+1] = 0.3*x1+u1, x2[k+1] = -x1+0.5*x2+((7)/(18))*x1**2+u2","source":"paper System 12; canonical record D... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\m... |
DCB-LIT-P1-013 | 13 | stability | Stability certification | literature | 3 | continuous | dx1/dt = -3*x1**3+3*x1*x3-9*x1, dx2/dt = -x1**3-5*x2+5*x3**3, dx3/dt = -9*x3**3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -3x_1^3+3x_1x_3-9x_1\\ -x_1^3-5x_2+5x_3^3\\ -9x_3^3 \end{pmatrix}. \] | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_013","task_type":"stability","name":"DynaCertBench System 013 · DCB-LIT-P1-013 · Table~1 row~4, \\cite{zou2025analytical}","dynamics":"dx1/dt = -3*x1**3+3*x1*x3-9*x1, dx2/dt = -x1**3-5*x2+5*x3**3, dx3/dt = -9*x3**3","source":"paper System 13; canonical record DCB-LIT-P1-013","assumptions":["De... | {"record_id":"DCB-LIT-P1-013","problem":{"problem_id":"dcb_lit_p1_013","task_type":"stability","name":"DynaCertBench System 013 · DCB-LIT-P1-013 · Table~1 row~4, \\cite{zou2025analytical}","dynamics":"dx1/dt = -3*x1**3+3*x1*x3-9*x1, dx2/dt = -x1**3-5*x2+5*x3**3, dx3/dt = -9*x3**3","source":"paper System 13; canonical r... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\... |
DCB-LIT-P1-014 | 14 | stability | Stability certification | literature | 3 | continuous | dx1/dt = x2, dx2/dt = -sin(x1)*cos(x1)-x2-sin(x3)*cos(x3), dx3/dt = x2-x3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} x_2\\ -\sin(x_1)\cos(x_1)-x_2-\sin(x_3)\cos(x_3)\\ x_2-x_3 \end{pmatrix}. \] | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_014","task_type":"stability","name":"DynaCertBench System 014 · DCB-LIT-P1-014 · Table~1 row~5, \\cite{zou2025analytical}","dynamics":"dx1/dt = x2, dx2/dt = -sin(x1)*cos(x1)-x2-sin(x3)*cos(x3), dx3/dt = x2-x3","source":"paper System 14; canonical record DCB-LIT-P1-014","assumptions":["Determin... | {"record_id":"DCB-LIT-P1-014","problem":{"problem_id":"dcb_lit_p1_014","task_type":"stability","name":"DynaCertBench System 014 · DCB-LIT-P1-014 · Table~1 row~5, \\cite{zou2025analytical}","dynamics":"dx1/dt = x2, dx2/dt = -sin(x1)*cos(x1)-x2-sin(x3)*cos(x3), dx3/dt = x2-x3","source":"paper System 14; canonical record ... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x}\\in\... |
DCB-LIT-P1-015 | 15 | stability | Stability certification | literature | 4 | continuous | dq/dt = w1-w2, dw1/dt = (1/2)*(-1-2*w1-sin(q)+cos(q)), dw2/dt = (1/2)*(-1-2*w2+sin(q)+cos(q)) | The source system is expressed in the center-of-inertia coordinates $(\delta_1,\delta_2,\omega_1,\omega_2)$, which satisfy $\delta_1+\delta_2=0$. We therefore remove the redundant common-angle coordinate and define $q:=\delta_1-\delta_2, \delta_1=\frac{q}{2}, \delta_2=-\frac{q}{2}$. Let $\mathbf{x}=(q,\omega_1,\omega_2... | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_015","task_type":"stability","name":"DynaCertBench System 015 · DCB-LIT-P1-015 · Table~1 row~6, \\cite{zou2025analytical}","dynamics":"dq/dt = w1-w2, dw1/dt = (1/2)*(-1-2*w1-sin(q)+cos(q)), dw2/dt = (1/2)*(-1-2*w2+sin(q)+cos(q))","source":"paper System 15; canonical record DCB-LIT-P1-015","ass... | {"record_id":"DCB-LIT-P1-015","problem":{"problem_id":"dcb_lit_p1_015","task_type":"stability","name":"DynaCertBench System 015 · DCB-LIT-P1-015 · Table~1 row~6, \\cite{zou2025analytical}","dynamics":"dq/dt = w1-w2, dw1/dt = (1/2)*(-1-2*w1-sin(q)+cos(q)), dw2/dt = (1/2)*(-1-2*w2+sin(q)+cos(q))","source":"paper System 1... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $ \\mathcal{N} = \\left\\{ (q,\\o... |
DCB-LIT-P1-016 | 16 | stability | Stability certification | literature | 6 | continuous | dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt = -x5+0.5*x6, dx6/dt = -0.5*x5-x6+0.1*x2**2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3\\ \dot{x}_4\\ \dot{x}_5\\ \dot{x}_6 \end{pmatrix} = \begin{pmatrix} -x_1+0.5x_2-0.1x_5^2\\ -0.5x_1-x_2\\ -x_3+0.5x_4-0.1x_1^2\\ -0.5x_3-x_4\\ -x_5+0.5x_6\\ -0.5x_5-x_6+0.1x_2^2 \end{pmatrix}. \] | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_016","task_type":"stability","name":"DynaCertBench System 016 · DCB-LIT-P1-016 · Table~1 row~7, \\cite{zou2025analytical}","dynamics":"dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt = -x5+0.5*x6, dx6/dt = -0.5*x5-x6+0.1*x2**2","so... | {"record_id":"DCB-LIT-P1-016","problem":{"problem_id":"dcb_lit_p1_016","task_type":"stability","name":"DynaCertBench System 016 · DCB-LIT-P1-016 · Table~1 row~7, \\cite{zou2025analytical}","dynamics":"dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt = -x5+0.... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0,0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x... |
DCB-LIT-P1-017 | 17 | stability | Stability certification | literature | 6 | continuous | dx1/dt = x2, dx2/dt = -((3)/(2))*x6*x4-2*x1-((5)/(2))*x2-((1)/(2))*x4*sin(x2)*cos(x4), dx3/dt = x4, dx4/dt = ((3)/(2))*x6*x2-2*x3-10*x4+((1)/(2))*x2*sin(x2)*cos(x4), dx5/dt = x6, dx6/dt = -5*x5-((4)/(5))*x6 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3\\ \dot{x}_4\\ \dot{x}_5\\ \dot{x}_6 \end{pmatrix} = \begin{pmatrix} x_2\\ -\tfrac32x_6x_4-2x_1-\tfrac52x_2-\tfrac12x_4\sin(x_2)\cos(x_4)\\ x_4\\ \tfrac32x_6x_2-2x_3-10x_4+\tfrac12x_2\sin(x_2)\cos(x_4)\\ x_6\\ -5x_5-\tfrac4... | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_017","task_type":"stability","name":"DynaCertBench System 017 · DCB-LIT-P1-017 · Table~1 row~8, \\cite{zou2025analytical}","dynamics":"dx1/dt = x2, dx2/dt = -((3)/(2))*x6*x4-2*x1-((5)/(2))*x2-((1)/(2))*x4*sin(x2)*cos(x4), dx3/dt = x4, dx4/dt = ((3)/(2))*x6*x2-2*x3-10*x4+((1)/(2))*x2*sin(x2)*co... | {"record_id":"DCB-LIT-P1-017","problem":{"problem_id":"dcb_lit_p1_017","task_type":"stability","name":"DynaCertBench System 017 · DCB-LIT-P1-017 · Table~1 row~8, \\cite{zou2025analytical}","dynamics":"dx1/dt = x2, dx2/dt = -((3)/(2))*x6*x4-2*x1-((5)/(2))*x2-((1)/(2))*x4*sin(x2)*cos(x4), dx3/dt = x4, dx4/dt = ((3)/(2))*... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0,0,0,0)$","Original $\\mathcal{N}=\\{\\mathbf{x... |
DCB-LIT-P1-018 | 18 | stability | Stability certification | literature | 6 | continuous | dd1/dt = w1-(w1+w2+w3)/3, dd2/dt = w2-(w1+w2+w3)/3, dw1/dt = -w1-(1/2)*(sin(d1-d2)+sin(2*d1+d2)), dw2/dt = -w2-(1/2)*(sin(d2-d1)+sin(d1+2*d2)), dw3/dt = -w3+(1/2)*(sin(2*d1+d2)+sin(d1+2*d2)) | The source system is expressed in the center-of-inertia coordinates $(\delta_1,\delta_2,\delta_3,\omega_1,\omega_2,\omega_3)$, which satisfy $\delta_1+\delta_2+\delta_3=0$. We therefore remove the redundant common-angle coordinate and define $\delta_3:=-(\delta_1+\delta_2)$ and $\bar{\omega}:=\frac13(\omega_1+\omega_2+... | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_018","task_type":"stability","name":"DynaCertBench System 018 · DCB-LIT-P1-018 · Table~1 row~9, \\cite{zou2025analytical}","dynamics":"dd1/dt = w1-(w1+w2+w3)/3, dd2/dt = w2-(w1+w2+w3)/3, dw1/dt = -w1-(1/2)*(sin(d1-d2)+sin(2*d1+d2)), dw2/dt = -w2-(1/2)*(sin(d2-d1)+sin(d1+2*d2)), dw3/dt = -w3+(1... | {"record_id":"DCB-LIT-P1-018","problem":{"problem_id":"dcb_lit_p1_018","task_type":"stability","name":"DynaCertBench System 018 · DCB-LIT-P1-018 · Table~1 row~9, \\cite{zou2025analytical}","dynamics":"dd1/dt = w1-(w1+w2+w3)/3, dd2/dt = w2-(w1+w2+w3)/3, dw1/dt = -w1-(1/2)*(sin(d1-d2)+sin(2*d1+d2)), dw2/dt = -w2-(1/2)*(s... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0,0,0)$","Original $\\mathcal{N} = \\{(\\delta_1... |
DCB-LIT-P1-019 | 19 | stability | Stability certification | literature | 9 | continuous | dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2+0.1*x8, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt = -x5+0.5*x6, dx6/dt = -0.5*x5-x6+0.1*x2**2, dx7/dt = x8, dx8/dt = -sin(x7)*cos(x7)-x8-sin(x9)*cos(x9)-0.1*x2, dx9/dt = x8-x9 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3\\ \dot{x}_4\\ \dot{x}_5\\ \dot{x}_6\\ \dot{x}_7\\ \dot{x}_8\\ \dot{x}_9 \end{pmatrix} = \begin{pmatrix} -x_1+0.5x_2-0.1x_5^2\\ -0.5x_1-x_2+0.1x_8\\ -x_3+0.5x_4-0.1x_1^2\\ -0.5x_3-x_4\\ -x_5+0.5x_6\\ -0.5x_5-x_6+0.1x_2^2\\ ... | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_019","task_type":"stability","name":"DynaCertBench System 019 · DCB-LIT-P1-019 · Table~1 row~10, \\cite{zou2025analytical}","dynamics":"dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2+0.1*x8, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt = -x5+0.5*x6, dx6/dt = -0.5*x5-x6+0.1*x2... | {"record_id":"DCB-LIT-P1-019","problem":{"problem_id":"dcb_lit_p1_019","task_type":"stability","name":"DynaCertBench System 019 · DCB-LIT-P1-019 · Table~1 row~10, \\cite{zou2025analytical}","dynamics":"dx1/dt = -x1+0.5*x2-0.1*x5**2, dx2/dt = -0.5*x1-x2+0.1*x8, dx3/dt = -x3+0.5*x4-0.1*x1**2, dx4/dt = -0.5*x3-x4, dx5/dt ... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0,0,0,0,0,0,0,0)$","Original $\\mathcal{N}=\\{\\ma... |
DCB-LIT-P1-020 | 20 | stability | Stability certification | literature | 3 | continuous | dx1/dt = -8*x1*x2**2-10*x2**4, dx2/dt = -8*x2**3+3*x2**2-8*x2, dx3/dt = -x3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -8x_1x_2^2-10x_2^4\\ -8x_2^3+3x_2^2-8x_2\\ -x_3 \end{pmatrix}. \] | [
"zou2025analytical"
] | {"problem_id":"dcb_lit_p1_020","task_type":"stability","name":"DynaCertBench System 020 · DCB-LIT-P1-020 · Appendix Table~6, \\cite{zou2025analytical}","dynamics":"dx1/dt = -8*x1*x2**2-10*x2**4, dx2/dt = -8*x2**3+3*x2**2-8*x2, dx3/dt = -x3","source":"paper System 20; canonical record DCB-LIT-P1-020","assumptions":["Det... | {"record_id":"DCB-LIT-P1-020","problem":{"problem_id":"dcb_lit_p1_020","task_type":"stability","name":"DynaCertBench System 020 · DCB-LIT-P1-020 · Appendix Table~6, \\cite{zou2025analytical}","dynamics":"dx1/dt = -8*x1*x2**2-10*x2**4, dx2/dt = -8*x2**3+3*x2**2-8*x2, dx3/dt = -x3","source":"paper System 20; canonical re... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["Original $\\mathcal{N}=\\{\\mathbf{x}\\in\\mathbb{R}^{3}\\mid e... |
DCB-LIT-P1-021 | 21 | stability | Stability certification | literature | 2 | continuous | dx1/dt = 4*x1**3-x1**2*x2-6*x1*x2**2-x2**3, dx2/dt = x1**3+4*x1**2*x2+x1*x2**2-6*x2**3 | The vector flow field is: \[ \dot{\mathbf{x}}= \begin{pmatrix}\dot{x}\\\dot{y}\end{pmatrix} = \begin{pmatrix}4x^3-x^2y-6xy^2-y^3\\x^3+4x^2y+xy^2-6y^3\end{pmatrix}. \] | [
"liu2026globally"
] | {"problem_id":"dcb_lit_p1_021","task_type":"stability","name":"DynaCertBench System 021 · DCB-LIT-P1-021 · Main theorem, \\cite{liu2026globally}","dynamics":"dx1/dt = 4*x1**3-x1**2*x2-6*x1*x2**2-x2**3, dx2/dt = x1**3+4*x1**2*x2+x1*x2**2-6*x2**3","source":"paper System 21; canonical record DCB-LIT-P1-021","assumptions":... | {"record_id":"DCB-LIT-P1-021","problem":{"problem_id":"dcb_lit_p1_021","task_type":"stability","name":"DynaCertBench System 021 · DCB-LIT-P1-021 · Main theorem, \\cite{liu2026globally}","dynamics":"dx1/dt = 4*x1**3-x1**2*x2-6*x1*x2**2-x2**3, dx2/dt = x1**3+4*x1**2*x2+x1*x2**2-6*x2**3","source":"paper System 21; canonic... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":1,"problem_name":"Stability certification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\mathbb{R}^{2}$","Or... |
DCB-LIT-P2-001 | 22 | roa | Region-of-attraction verification | literature | 2 | continuous | dx1/dt = x2, dx2/dt = ((3/20)*(981/100)*(1/2)*sin(x1)+(20*tanh(-(23286329/1000000)*x1-(105411/20000)*x2))-(1/10)*x2)/((3/20)*(1/2)**2) | The closed-loop vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{\theta}\\ \dot{\omega} \end{pmatrix} = \begin{pmatrix} \omega\\ \dfrac{mg\ell\sin(\theta)+u-0.1\omega}{m\ell^2} \end{pmatrix}. \] \[ u=20\tanh(-23.286329\theta-5.27055\omega), \] where $m=0.15,\ell=0.5$ and $g=9.81$. | [
"zhou2022neural"
] | {"problem_id":"dcb_lit_p2_001","task_type":"roa","name":"DynaCertBench System 022 · DCB-LIT-P2-001 · Section~5.3 and Appendix~C.3.3, \\cite{zhou2022neural}","dynamics":"dx1/dt = x2, dx2/dt = ((3/20)*(981/100)*(1/2)*sin(x1)+(20*tanh(-(23286329/1000000)*x1-(105411/20000)*x2))-(1/10)*x2)/((3/20)*(1/2)**2)","source":"paper... | {"record_id":"DCB-LIT-P2-001","problem":{"problem_id":"dcb_lit_p2_001","task_type":"roa","name":"DynaCertBench System 022 · DCB-LIT-P2-001 · Section~5.3 and Appendix~C.3.3, \\cite{zhou2022neural}","dynamics":"dx1/dt = x2, dx2/dt = ((3/20)*(981/100)*(1/2)*sin(x1)+(20*tanh(-(23286329/1000000)*x1-(105411/20000)*x2))-(1/10... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf... |
DCB-LIT-P2-002 | 23 | roa | Region-of-attraction verification | literature | 2 | continuous | dx1/dt = -x2, dx2/dt = x1 + (x1**2 - 1)*x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} -x_2\\ x_1+(x_1^2-1)x_2 \end{pmatrix}. \] | [
"zhou2022neural"
] | {"problem_id":"dcb_lit_p2_002","task_type":"roa","name":"DynaCertBench System 023 · DCB-LIT-P2-002 · Section~5.1 and Appendix~C.3.1, \\cite{zhou2022neural}","dynamics":"dx1/dt = -x2, dx2/dt = x1 + (x1**2 - 1)*x2","equilibrium":[0,0],"stability_kind":"local_asymptotic","neighborhood":{"type":"ball","center":[0,0],"radiu... | {"record_id":"DCB-LIT-P2-002","problem":{"problem_id":"dcb_lit_p2_002","task_type":"roa","name":"DynaCertBench System 023 · DCB-LIT-P2-002 · Section~5.1 and Appendix~C.3.1, \\cite{zhou2022neural}","dynamics":"dx1/dt = -x2, dx2/dt = x1 + (x1**2 - 1)*x2","equilibrium":[0,0],"stability_kind":"local_asymptotic","neighborho... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=\\{\\mathbf... |
DCB-LIT-P2-003 | 24 | roa | Region-of-attraction verification | literature | 1 | continuous | dx/dt = -x + x**3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x} \end{pmatrix} = \begin{pmatrix} -x+x^3 \end{pmatrix}. \] | [
"liu2023towards"
] | {"problem_id":"dcb_lit_p2_003","task_type":"roa","name":"DynaCertBench System 024 · DCB-LIT-P2-003 · Example~3.1, \\cite{liu2023towards}","dynamics":"dx/dt = -x + x**3","equilibrium":[0],"stability_kind":"local_asymptotic","neighborhood":{"type":"constraint","lhs":"x**2","relation":"lt","rhs":"1","bounds":[[-1,1]]},"an... | {"record_id":"DCB-LIT-P2-003","problem":{"problem_id":"dcb_lit_p2_003","task_type":"roa","name":"DynaCertBench System 024 · DCB-LIT-P2-003 · Example~3.1, \\cite{liu2023towards}","dynamics":"dx/dt = -x + x**3","equilibrium":[0],"stability_kind":"local_asymptotic","neighborhood":{"type":"constraint","lhs":"x**2","relatio... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=0$","Original $\\mathcal{N}=(-1,1)$","Origi... |
DCB-LIT-P2-004 | 25 | roa | Region-of-attraction verification | literature | 2 | continuous | dx1/dt = x2, dx2/dt = -2*x1 + 1/3*x1**3 - x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} x_2\\ -2x_1+\tfrac13x_1^3-x_2 \end{pmatrix}. \] | [
"liu2023towards"
] | {"problem_id":"dcb_lit_p2_004","task_type":"roa","name":"DynaCertBench System 025 · DCB-LIT-P2-004 · Example~6.2 and Table~II, \\cite{liu2023towards}","dynamics":"dx1/dt = x2, dx2/dt = -2*x1 + 1/3*x1**3 - x2","equilibrium":[0,0],"stability_kind":"local_asymptotic","neighborhood":{"type":"box","bounds":[[-6,6],[-6,6]]},... | {"record_id":"DCB-LIT-P2-004","problem":{"problem_id":"dcb_lit_p2_004","task_type":"roa","name":"DynaCertBench System 025 · DCB-LIT-P2-004 · Example~6.2 and Table~II, \\cite{liu2023towards}","dynamics":"dx1/dt = x2, dx2/dt = -2*x1 + 1/3*x1**3 - x2","equilibrium":[0,0],"stability_kind":"local_asymptotic","neighborhood":... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=[-6,6]^2$",... |
DCB-LIT-P2-005 | 26 | roa | Region-of-attraction verification | literature | 3 | continuous | dx1/dt = -10*(x1-x2) + u1, dx2/dt = 28*x1 - x2 - x1*x3 + u2, dx3/dt = x1*x2 - 8/3*x3 + u3 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3 \end{pmatrix} = \begin{pmatrix} -10(x_1-x_2)+u_1\\ 28x_1-x_2-x_1x_3+u_2\\ x_1x_2-\dfrac83x_3+u_3 \end{pmatrix}. \] | [
"edwards2024fossil"
] | {"problem_id":"dcb_lit_p2_005","task_type":"roa","name":"DynaCertBench System 026 · DCB-LIT-P2-005 · Table~4 \\#3 (LorenzSystem), \\cite{edwards2024fossil}","dynamics":"dx1/dt = -10*(x1-x2) + u1, dx2/dt = 28*x1 - x2 - x1*x3 + u2, dx3/dt = x1*x2 - 8/3*x3 + u3","controller_parameters":"u1,u2,u3","equilibrium":[0,0,0],"st... | {"record_id":"DCB-LIT-P2-005","problem":{"problem_id":"dcb_lit_p2_005","task_type":"roa","name":"DynaCertBench System 026 · DCB-LIT-P2-005 · Table~4 \\#3 (LorenzSystem), \\cite{edwards2024fossil}","dynamics":"dx1/dt = -10*(x1-x2) + u1, dx2/dt = 28*x1 - x2 - x1*x3 + u2, dx3/dt = x1*x2 - 8/3*x3 + u3","controller_paramete... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","initial_set_X_I","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=(0,0,0)$","Original $\\ma... |
DCB-LIT-P2-006 | 27 | roa | Region-of-attraction verification | literature | 2 | continuous | dx1/dt = x2, dx2/dt = -1/2*x2-sin(x1+pi/3)+sin(pi/3) | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} x_2\\ -0.5x_2-\sin\left(x_1+\dfrac{\pi}{3}\right) +\sin\left(\dfrac{\pi}{3}\right) \end{pmatrix}. \] | [
"liu2024tool"
] | {"problem_id":"dcb_lit_p2_006","task_type":"roa","name":"DynaCertBench System 027 · DCB-LIT-P2-006 · Example~5.2 and Table~2, \\cite{liu2024tool}","dynamics":"dx1/dt = x2, dx2/dt = -1/2*x2-sin(x1+pi/3)+sin(pi/3)","source":"paper System 27; canonical record DCB-LIT-P2-006","assumptions":["Transcribed from paper-4-20-202... | {"record_id":"DCB-LIT-P2-006","paper_system_number":27,"paper_system_label":"System 27","local_name":"S027__DCB-LIT-P2-006","problem":{"problem_id":"dcb_lit_p2_006","task_type":"roa","name":"DynaCertBench System 027 · DCB-LIT-P2-006 · Example~5.2 and Table~2, \\cite{liu2024tool}","dynamics":"dx1/dt = x2, dx2/dt = -1/2*... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=(0,0)$","Original $\\mathcal{N}=[-2,3]\\tim... |
DCB-LIT-P2-007 | 28 | roa | Region-of-attraction verification | literature | 10 | continuous | dx1/dt = -x1 + 1/2*x2 - 1/10*x9**2, dx2/dt = -1/2*x1 - x2, dx3/dt = -x3 + 1/2*x4 - 1/10*x1**2, dx4/dt = -1/2*x3 - x4, dx5/dt = -x5 + 1/2*x6 + 1/10*x7**2, dx6/dt = -1/2*x5 - x6, dx7/dt = -x7 + 1/2*x8, dx8/dt = -1/2*x7 - x8, dx9/dt = -x9 + 1/2*x10, dx10/dt = -1/2*x9 - x10 + 1/10*x2**2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2\\ \dot{x}_3\\ \dot{x}_4\\ \dot{x}_5\\ \dot{x}_6\\ \dot{x}_7\\ \dot{x}_8\\ \dot{x}_9\\ \dot{x}_{10} \end{pmatrix} = \begin{pmatrix} -x_1+0.5x_2-0.1x_9^2\\ -0.5x_1-x_2\\ -x_3+0.5x_4-0.1x_1^2\\ -0.5x_3-x_4\\ -x_5+0.5x_6+0.1x_7^2\\ -0.5x_... | [
"liu2024tool"
] | {"problem_id":"dcb_lit_p2_007","task_type":"roa","name":"DynaCertBench System 028 · DCB-LIT-P2-007 · Example~5.4 and Table~3, \\cite{liu2024tool}","dynamics":"dx1/dt = -x1 + 1/2*x2 - 1/10*x9**2, dx2/dt = -1/2*x1 - x2, dx3/dt = -x3 + 1/2*x4 - 1/10*x1**2, dx4/dt = -1/2*x3 - x4, dx5/dt = -x5 + 1/2*x6 + 1/10*x7**2, dx6/dt ... | {"record_id":"DCB-LIT-P2-007","problem":{"problem_id":"dcb_lit_p2_007","task_type":"roa","name":"DynaCertBench System 028 · DCB-LIT-P2-007 · Example~5.4 and Table~3, \\cite{liu2024tool}","dynamics":"dx1/dt = -x1 + 1/2*x2 - 1/10*x9**2, dx2/dt = -1/2*x1 - x2, dx3/dt = -x3 + 1/2*x4 - 1/10*x1**2, dx4/dt = -1/2*x3 - x4, dx5... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["$x^\\star=\\mathbf{0}$","Original $\\mathcal{N}=[-1,1... |
DCB-LIT-P2-008 | 29 | roa | Region-of-attraction verification | literature | 1 | continuous | dx/dt = -x - x**3 | The closed-loop scalar dynamics are: \[ \dot{x}=-x-x^3, \] | [
"meng2024physics"
] | {"problem_id":"dcb_lit_p2_008","task_type":"roa","name":"DynaCertBench System 029 · DCB-LIT-P2-008 · Section~5.1, with verification details in Appendix~E.2 (\\(n=1\\)), \\cite{meng2024physics}","dynamics":"dx/dt = -x - x**3","equilibrium":[0],"stability_kind":"local_asymptotic","neighborhood":{"type":"box","bounds":[[-... | {"record_id":"DCB-LIT-P2-008","problem":{"problem_id":"dcb_lit_p2_008","task_type":"roa","name":"DynaCertBench System 029 · DCB-LIT-P2-008 · Section~5.1, with verification details in Appendix~E.2 (\\(n=1\\)), \\cite{meng2024physics}","dynamics":"dx/dt = -x - x**3","equilibrium":[0],"stability_kind":"local_asymptotic","... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["equilibrium","neighborhood_N"],"set_contract_complete":true},"problem":2,"problem_name":"Region-of-attraction verification","raw_items_latex":["Equilibrium: $x^\\star=0$","Original $ \\mathcal{N} =... |
DCB-LIT-P3-001 | 30 | invariant | Forward-invariant set synthesis | literature | 6 | discrete | x1[k+1] = x1+1/20*(x4*cos(x3)-x5*sin(x3)), x2[k+1] = x2+1/20*(x4*sin(x3)+x5*cos(x3)), x3[k+1] = x3+1/20*x6, x4[k+1] = x4+1/20*(x5*x6-49/5*sin(x3)), x5[k+1] = x5+1/20*(-x4*x6-49/5*cos(x3)+(u1+u2)/4), x6[k+1] = x6+1/20*((1/4)/(19/400)*(u1-u2)) | Let the state be ordered as \[ \mathbf{x} = (p_x,p_z,\phi,v_x,v_z,\omega)^\top \in \mathbb{R}^{6}, \] where $(p_x,p_z)$ are the planar position, $\phi$ is the roll angle, $(v_x,v_z)$ are the body-frame velocities, and $\omega$ is the angular rate. Using the sampling period $\Delta t=0.05$, the discrete-time transition ... | [
"wu2023neural"
] | {"problem_id":"dcb_lit_p3_001","task_type":"invariant","name":"DynaCertBench System 030 · DCB-LIT-P3-001 · Appendix~A.1 (PVTOL), \\cite{wu2023neural}","dynamics":"x1[k+1] = x1+1/20*(x4*cos(x3)-x5*sin(x3)), x2[k+1] = x2+1/20*(x4*sin(x3)+x5*cos(x3)), x3[k+1] = x3+1/20*x6, x4[k+1] = x4+1/20*(x5*x6-49/5*sin(x3)), x5[k+1] =... | {"record_id":"DCB-LIT-P3-001","problem":{"problem_id":"dcb_lit_p3_001","task_type":"invariant","name":"DynaCertBench System 030 · DCB-LIT-P3-001 · Appendix~A.1 (PVTOL), \\cite{wu2023neural}","dynamics":"x1[k+1] = x1+1/20*(x4*cos(x3)-x5*sin(x3)), x2[k+1] = x2+1/20*(x4*sin(x3)+x5*cos(x3)), x3[k+1] = x3+1/20*x6, x4[k+1] =... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["state_space_X","unsafe_set_X_U"],"set_contract_complete":true},"problem":3,"problem_name":"Forward-invariant set synthesis","raw_items_latex":["$ \\mathcal{X} = \\left\\{ \\mathbf{x}\\in\\mathbb{R}... |
DCB-LIT-P3-002 | 31 | invariant | Forward-invariant set synthesis | literature | 2 | continuous | dx1/dt = x2, dx2/dt = sin(x1)-3*x1-3*x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_1\\ \dot{x}_2 \end{pmatrix} = \begin{pmatrix} x_2\\[1ex] \sin(x_1) + u \end{pmatrix}, \] where $u = -3x_1 - 3x_2$. | [
"samanipour2026relu"
] | {"problem_id":"dcb_lit_p3_002","task_type":"invariant","name":"DynaCertBench System 031 · DCB-LIT-P3-002 · Example~1, \\cite{samanipour2026relu}","dynamics":"dx1/dt = x2, dx2/dt = sin(x1)-3*x1-3*x2","source":"paper System 31; canonical record DCB-LIT-P3-002","assumptions":["Deterministically normalized from canonical r... | {"record_id":"DCB-LIT-P3-002","problem":{"problem_id":"dcb_lit_p3_002","task_type":"invariant","name":"DynaCertBench System 031 · DCB-LIT-P3-002 · Example~1, \\cite{samanipour2026relu}","dynamics":"dx1/dt = x2, dx2/dt = sin(x1)-3*x1-3*x2","source":"paper System 31; canonical record DCB-LIT-P3-002","assumptions":["Deter... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["state_space_X","unsafe_set_X_U"],"set_contract_complete":true},"problem":3,"problem_name":"Forward-invariant set synthesis","raw_items_latex":["$\\mathcal{X} = \\{x\\in\\mathbb{R}^{2}\\mid \\lVert ... |
DCB-LIT-P3-003 | 32 | invariant | Forward-invariant set synthesis | literature | 2 | continuous | dx1/dt = x1**2+x1*x2+x1, dx2/dt = x1*x2+x2**2+x2 | The vector flow field is: \[ \dot{\mathbf{x}} = \begin{pmatrix} \dot{x}_{1}\\ \dot{x}_{2} \end{pmatrix} = \begin{pmatrix} x_{1}^2 + x_{1}x_{2} + x_{1}\\[1ex] x_{1}x_{2} + x_{2}^2 + x_{2} \end{pmatrix}. \] | [
"samanipour2026relu"
] | {"problem_id":"dcb_lit_p3_003","task_type":"invariant","name":"DynaCertBench System 032 · DCB-LIT-P3-003 · Example~2, \\cite{samanipour2026relu}","dynamics":"dx1/dt = x1**2+x1*x2+x1, dx2/dt = x1*x2+x2**2+x2","source":"paper System 32; canonical record DCB-LIT-P3-003","assumptions":["Deterministically normalized from ca... | {"record_id":"DCB-LIT-P3-003","problem":{"problem_id":"dcb_lit_p3_003","task_type":"invariant","name":"DynaCertBench System 032 · DCB-LIT-P3-003 · Example~2, \\cite{samanipour2026relu}","dynamics":"dx1/dt = x1**2+x1*x2+x1, dx2/dt = x1*x2+x2**2+x2","source":"paper System 32; canonical record DCB-LIT-P3-003","assumptions... | {"candidate":null,"completeness":{"flags":[],"llm_input_ready":true,"missing_required_set_roles":[],"required_set_roles":["state_space_X","unsafe_set_X_U"],"set_contract_complete":true},"problem":3,"problem_name":"Forward-invariant set synthesis","raw_items_latex":["$\\mathcal{X} = \\{x\\in\\mathbb{R}^{2}\\mid \\lVert ... |
DynaCertBench
DynaCertBench contains 105 dynamical-system certification problems for evaluating certificate synthesis and verification. It accompanies LLM2Cert: LLM Synthesis of Certificates with SMT/Lean Verification.
Contents
| Task | Value of task_type |
Problems |
|---|---|---|
| Stability certification | stability |
26 |
| Region-of-attraction verification | roa |
12 |
| Forward-invariant set synthesis | invariant |
13 |
| Safety verification | safety |
54 |
| Total | 105 |
The benchmark includes 80 literature-derived problems (literature), 11 extended problems (extended), and 14 new systems (ours). There are 90 continuous-time and 15 discrete-time problems; the recorded system dimensions range from 1 to 10.
This distribution contains benchmark questions. All original candidate fields are null. Model outputs, proof answers, and experiment execution records are outside this dataset distribution.
Load the dataset
import json
from datasets import load_dataset
dataset = load_dataset("FormalCert-AI/DynaCertBench")
problems = dataset["test"]
assert len(problems) == 105
row = problems[0]
problem = json.loads(row["problem_json"])
original_record = json.loads(row["executable_record_json"])
description = json.loads(row["descriptive_record_json"])
stability_problems = problems.filter(lambda row: row["task_type"] == "stability")
All 105 problems are exposed in a single test split for evaluation. This packaging does not introduce a training/validation partition or assert that these public problems are held out from model training.
Fields
Each row corresponds to one original executable record, in the original order.
| Field | Meaning |
|---|---|
record_id |
Canonical problem identifier, e.g. DCB-LIT-P1-001 |
paper_system_number |
System number in the paper |
task_type |
stability, roa, invariant, or safety |
problem_name |
Task description from the descriptive source |
tier |
literature, extended, or ours |
dimension |
Recorded state dimension |
time_domain |
continuous or discrete |
dynamics |
Original executable dynamics string |
specification_latex |
Original descriptive system specification |
citations |
Source citation keys, preserved from the descriptive record |
problem_json |
Complete original executable problem object, serialized as JSON |
executable_record_json |
Complete original executable record, serialized as JSON |
descriptive_record_json |
Complete original descriptive record, serialized as JSON |
The JSON string fields preserve heterogeneous task schemas without dropping fields or converting numeric expressions. Use json.loads to recover the original objects. Display columns are copied from source fields; the serialized objects and original files remain the authoritative representations.
Original files and reproducibility
original/ contains byte-for-byte copies from GitHub commit 37b6a0484fc8b532bb29588b56f5993193c42fcc:
dynacertbench_executable.json: complete inputs consumed by the LLM2Cert pipeline.dynacertbench_by_problem.json: grouped descriptions, source references, metadata, and problem definitions.benchmark_curation_counts.json: aggregate curation counts; this is not a second set of benchmark problems.README.md: original dataset directory documentation.
provenance.json records the repository, pinned commit, Git blob hashes, SHA-256 checksums, and conversion policy. The original JSON files can also be downloaded directly:
import json
from huggingface_hub import hf_hub_download
path = hf_hub_download(
repo_id="FormalCert-AI/DynaCertBench",
filename="original/dynacertbench_executable.json",
repo_type="dataset",
)
with open(path, encoding="utf-8") as f:
executable = json.load(f)
Intended use and limitations
Use the dataset to evaluate synthesis of Lyapunov functions, barrier certificates, and related policies and their verification. The dataset itself does not execute a verifier or establish a new proof. Consult the original problem assumptions, formal contracts, and the LLM2Cert repository when running experiments.
The descriptive data preserves source-status annotations such as documented, inferred, and specified, and provenance placeholders such as <LOCAL_PATH> already present in the public GitHub release. These placeholders are not downloadable source files. Consult the source references when reusing an individual literature-derived problem. The source material and the executable normalization can express different roles (for example, original versus normalized neighborhoods); both representations are retained unchanged.
License and attribution
The source repository is released under the MIT license, reproduced in LICENSE. CITATION.cff and THIRD_PARTY_NOTICES.md are retained from that same public commit. Preserve the individual problem source citations when reusing the benchmark.
Citation
@misc{cao2026llm2cert,
title = {LLM2Cert: LLM Synthesis of Certificates with SMT/Lean Verification},
author = {Cao, Zhipeng and Song, Peiyang and Vertovec, Nikolaus and
Cui, Weiru and Yang, Zhihao and Liu, Mingkang and Lin, Luxia and
Xue, Bai and Abate, Alessandro},
year = {2026},
eprint = {2610.30524},
archivePrefix = {arXiv},
primaryClass = {eess.SY},
url = {https://arxiv.org/abs/2610.30524}
}
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