Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





Chosen Fixed Point

Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
55136 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_1\tilde{q}_2$ + $ M_5^2$ + $ \phi_1q_2^2$ + $ M_2M_3$ + $ M_6q_2\tilde{q}_1$ 0.7314 0.9189 0.796 [X:[], M:[0.7143, 1.0, 1.0, 0.7143, 1.0, 0.7143], q:[0.5, 0.7857], qb:[0.5, 0.5], phi:[0.4286]] [X:[], M:[[1], [1], [-1], [-1], [0], [0]], q:[[-1], [0]], qb:[[0], [1]], phi:[[0]]] 1 {a: 2007/2744, c: 5043/5488, M1: 5/7, M2: 1, M3: 1, M4: 5/7, M5: 1, M6: 5/7, q1: 1/2, q2: 11/14, qb1: 1/2, qb2: 1/2, phi1: 3/7}
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_1$, $ M_4$, $ M_6$, $ M_4$, $ M_1$, $ \phi_1^2$, $ M_2$, $ M_3$, $ M_5$, $ M_3$, $ M_2$, $ M_1^2$, $ M_1M_4$, $ M_4^2$, $ M_1M_6$, $ M_4M_6$, $ M_6^2$, $ \phi_1q_1^2$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ \phi_1q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ M_4^2$, $ \phi_1q_1^2$, $ M_4M_6$, $ \phi_1q_1\tilde{q}_1$, $ M_1M_6$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ M_1^2$, $ \phi_1\tilde{q}_2^2$, $ M_1\phi_1^2$, $ M_4\phi_1^2$, $ M_6\phi_1^2$, $ M_4\phi_1^2$, $ M_1\phi_1^2$, $ M_1M_2$, $ M_1M_3$, $ M_2M_4$, $ M_3M_4$, $ M_1M_5$, $ M_4M_5$, $ M_2M_6$, $ M_3M_6$, $ M_5M_6$, $ \phi_1^4$, $ \phi_1q_1q_2$, $ \phi_1q_2\tilde{q}_1$, $ \phi_1q_2\tilde{q}_2$, $ M_3M_4$, $ M_4M_5$, $ M_3M_6$, $ \phi_1q_1q_2$, $ M_1M_5$, $ M_2M_6$, $ \phi_1q_2\tilde{q}_2$, $ M_1M_2$, $ M_2\phi_1^2$, $ M_3\phi_1^2$, $ M_5\phi_1^2$, $ M_3\phi_1^2$, $ M_2\phi_1^2$ $M_2^2$, $ M_3^2$, $ M_2M_5$, $ M_3M_5$ -3 3*t^2.14 + t^2.57 + 3*t^3. + 12*t^4.29 + 3*t^4.71 + 10*t^5.14 + 3*t^5.57 - 3*t^6. + 25*t^6.43 + 8*t^6.86 + 28*t^7.29 + 4*t^7.71 - 14*t^8.14 + 51*t^8.57 - t^4.29/y - (3*t^6.43)/y - t^6.86/y + (3*t^7.29)/y + (4*t^7.71)/y + (12*t^8.14)/y - (3*t^8.57)/y - t^4.29*y - 3*t^6.43*y - t^6.86*y + 3*t^7.29*y + 4*t^7.71*y + 12*t^8.14*y - 3*t^8.57*y t^2.14 + t^2.14/g1 + g1*t^2.14 + t^2.57 + t^3. + t^3./g1 + g1*t^3. + 4*t^4.29 + (2*t^4.29)/g1^2 + (2*t^4.29)/g1 + 2*g1*t^4.29 + 2*g1^2*t^4.29 + t^4.71 + t^4.71/g1 + g1*t^4.71 + 4*t^5.14 + t^5.14/g1^2 + (2*t^5.14)/g1 + 2*g1*t^5.14 + g1^2*t^5.14 + t^5.57 + t^5.57/g1 + g1*t^5.57 - t^6. - t^6./g1 - g1*t^6. + 5*t^6.43 + (2*t^6.43)/g1^3 + (3*t^6.43)/g1^2 + (5*t^6.43)/g1 + 5*g1*t^6.43 + 3*g1^2*t^6.43 + 2*g1^3*t^6.43 + 2*t^6.86 + (2*t^6.86)/g1^2 + t^6.86/g1 + g1*t^6.86 + 2*g1^2*t^6.86 + 6*t^7.29 + (2*t^7.29)/g1^3 + (3*t^7.29)/g1^2 + (6*t^7.29)/g1 + 6*g1*t^7.29 + 3*g1^2*t^7.29 + 2*g1^3*t^7.29 + 2*t^7.71 + t^7.71/g1 + g1*t^7.71 - 4*t^8.14 - (2*t^8.14)/g1^2 - (3*t^8.14)/g1 - 3*g1*t^8.14 - 2*g1^2*t^8.14 + 9*t^8.57 + (3*t^8.57)/g1^4 + (4*t^8.57)/g1^3 + (8*t^8.57)/g1^2 + (6*t^8.57)/g1 + 6*g1*t^8.57 + 8*g1^2*t^8.57 + 4*g1^3*t^8.57 + 3*g1^4*t^8.57 - t^4.29/y - t^6.43/y - t^6.43/(g1*y) - (g1*t^6.43)/y - t^6.86/y + t^7.29/y + t^7.29/(g1*y) + (g1*t^7.29)/y + (2*t^7.71)/y + t^7.71/(g1*y) + (g1*t^7.71)/y + (4*t^8.14)/y + t^8.14/(g1^2*y) + (3*t^8.14)/(g1*y) + (3*g1*t^8.14)/y + (g1^2*t^8.14)/y - t^8.57/y - t^8.57/(g1^2*y) - (g1^2*t^8.57)/y - t^4.29*y - t^6.43*y - (t^6.43*y)/g1 - g1*t^6.43*y - t^6.86*y + t^7.29*y + (t^7.29*y)/g1 + g1*t^7.29*y + 2*t^7.71*y + (t^7.71*y)/g1 + g1*t^7.71*y + 4*t^8.14*y + (t^8.14*y)/g1^2 + (3*t^8.14*y)/g1 + 3*g1*t^8.14*y + g1^2*t^8.14*y - t^8.57*y - (t^8.57*y)/g1^2 - g1^2*t^8.57*y


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from the Same Seed Theory

Below is a list of equivalent fixed points from the same seed theories.

id Theory Superpotential Central Charge $a$ Central Charge $c$ Ratio $a/c$ $R$-charges More Info. Rational


Previous Theory

The previous fixed point before deforming to get the chosen fixed point.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
46856 SU2adj1nf2 $M_1q_1q_2$ + $ M_2q_1\tilde{q}_1$ + $ M_3\tilde{q}_1\tilde{q}_2$ + $ M_4q_2\tilde{q}_2$ + $ M_5q_1\tilde{q}_2$ + $ M_5^2$ + $ \phi_1q_2^2$ + $ M_2M_3$ 0.7112 0.8808 0.8074 [X:[], M:[0.7143, 1.0, 1.0, 0.7143, 1.0], q:[0.5, 0.7857], qb:[0.5, 0.5], phi:[0.4286]] 2*t^2.14 + t^2.57 + 3*t^3. + t^3.86 + 9*t^4.29 + 2*t^4.71 + 7*t^5.14 + 3*t^5.57 - t^6. - t^4.29/y - t^4.29*y detail {a: 3903/5488, c: 2417/2744, M1: 5/7, M2: 1, M3: 1, M4: 5/7, M5: 1, q1: 1/2, q2: 11/14, qb1: 1/2, qb2: 1/2, phi1: 3/7}