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
55511 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_2q_1\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2^2$ + $ M_6q_1q_2$ 0.6587 0.8488 0.776 [X:[], M:[1.1039, 0.75, 0.7922, 1.25, 0.7078, 0.8539], q:[0.75, 0.3961], qb:[0.3539, 0.5], phi:[0.5]] [X:[], M:[[1], [0], [-2], [0], [2], [1]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_5$, $ q_2\tilde{q}_1$, $ M_3$, $ M_6$, $ \tilde{q}_1\tilde{q}_2$, $ \phi_1^2$, $ M_1$, $ q_1\tilde{q}_1$, $ M_4$, $ q_1\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ \phi_1q_2\tilde{q}_2$, $ M_5^2$, $ M_5q_2\tilde{q}_1$, $ M_3M_5$, $ q_2^2\tilde{q}_1^2$, $ \phi_1\tilde{q}_2^2$, $ M_3q_2\tilde{q}_1$, $ M_5M_6$, $ M_5\tilde{q}_1\tilde{q}_2$, $ M_3^2$, $ M_6q_2\tilde{q}_1$, $ q_2\tilde{q}_1^2\tilde{q}_2$, $ M_3M_6$, $ M_3\tilde{q}_1\tilde{q}_2$, $ M_6^2$, $ M_5\phi_1^2$, $ M_6\tilde{q}_1\tilde{q}_2$, $ \tilde{q}_1^2\tilde{q}_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ M_3\phi_1^2$, $ M_1M_5$, $ M_5q_1\tilde{q}_1$, $ M_6\phi_1^2$, $ q_1q_2\tilde{q}_1^2$, $ \phi_1^2\tilde{q}_1\tilde{q}_2$, $ M_1M_3$, $ M_3q_1\tilde{q}_1$, $ M_4M_5$, $ M_1M_6$, $ M_6q_1\tilde{q}_1$, $ M_5q_1\tilde{q}_2$, $ q_1\tilde{q}_1^2\tilde{q}_2$ $M_4q_2\tilde{q}_1$ -1 t^2.12 + t^2.25 + t^2.38 + 2*t^2.56 + t^3. + 2*t^3.31 + 2*t^3.75 + t^4.06 + t^4.19 + t^4.25 + t^4.37 + 3*t^4.5 + t^4.63 + 2*t^4.68 + t^4.75 + 2*t^4.81 + 2*t^4.94 + 4*t^5.12 + t^5.25 + t^5.38 + 2*t^5.43 + 3*t^5.56 + t^5.69 + 5*t^5.87 - t^6. + t^6.13 + t^6.18 + 5*t^6.31 + t^6.37 - t^6.44 + t^6.5 + t^6.57 + 7*t^6.62 + 3*t^6.75 + 2*t^6.81 + 2*t^6.88 + 2*t^6.93 + t^7. + 7*t^7.06 + t^7.13 - t^7.19 + 4*t^7.25 + 2*t^7.32 + 4*t^7.37 + 5*t^7.5 + 2*t^7.56 - t^7.63 + 7*t^7.68 + t^7.75 + 4*t^7.81 + 5*t^8. + t^8.07 + 3*t^8.12 + 2*t^8.25 + t^8.31 - 2*t^8.38 + 9*t^8.43 + t^8.49 + t^8.5 - 3*t^8.56 + t^8.62 + t^8.69 + 7*t^8.75 - t^8.82 + 8*t^8.87 + 2*t^8.93 + t^8.94 - t^4.5/y - t^6.62/y - t^6.88/y - t^7.06/y + t^7.19/y + t^7.37/y + t^7.5/y + t^7.63/y + (2*t^7.68)/y + t^7.81/y + (3*t^7.94)/y + (3*t^8.12)/y + t^8.25/y + (2*t^8.38)/y + (2*t^8.43)/y + (4*t^8.56)/y + (2*t^8.69)/y - t^8.75/y + (6*t^8.87)/y - t^4.5*y - t^6.62*y - t^6.88*y - t^7.06*y + t^7.19*y + t^7.37*y + t^7.5*y + t^7.63*y + 2*t^7.68*y + t^7.81*y + 3*t^7.94*y + 3*t^8.12*y + t^8.25*y + 2*t^8.38*y + 2*t^8.43*y + 4*t^8.56*y + 2*t^8.69*y - t^8.75*y + 6*t^8.87*y g1^2*t^2.12 + t^2.25 + t^2.38/g1^2 + 2*g1*t^2.56 + t^3. + 2*g1*t^3.31 + 2*t^3.75 + g1*t^4.06 + t^4.19/g1 + g1^4*t^4.25 + g1^2*t^4.37 + 3*t^4.5 + t^4.63/g1^2 + 2*g1^3*t^4.68 + t^4.75/g1^4 + 2*g1*t^4.81 + (2*t^4.94)/g1 + 4*g1^2*t^5.12 + t^5.25 + t^5.38/g1^2 + 2*g1^3*t^5.43 + 3*g1*t^5.56 + t^5.69/g1 + 5*g1^2*t^5.87 - t^6. + t^6.13/g1^2 + g1^3*t^6.18 + 5*g1*t^6.31 + g1^6*t^6.37 - t^6.44/g1 + g1^4*t^6.5 + t^6.57/g1^3 + 7*g1^2*t^6.62 + 3*t^6.75 + 2*g1^5*t^6.81 + (2*t^6.88)/g1^2 + 2*g1^3*t^6.93 + t^7./g1^4 + 7*g1*t^7.06 + t^7.13/g1^6 - t^7.19/g1 + 4*g1^4*t^7.25 + (2*t^7.32)/g1^3 + 4*g1^2*t^7.37 + 5*t^7.5 + 2*g1^5*t^7.56 - t^7.63/g1^2 + 7*g1^3*t^7.68 + t^7.75/g1^4 + 4*g1*t^7.81 + 5*g1^4*t^8. + t^8.07/g1^3 + 3*g1^2*t^8.12 + 2*t^8.25 + g1^5*t^8.31 - (2*t^8.38)/g1^2 + 9*g1^3*t^8.43 + g1^8*t^8.49 + t^8.5/g1^4 - 3*g1*t^8.56 + g1^6*t^8.62 + t^8.69/g1 + 7*g1^4*t^8.75 - t^8.82/g1^3 + 8*g1^2*t^8.87 + 2*g1^7*t^8.93 + t^8.94/g1^5 - t^4.5/y - (g1^2*t^6.62)/y - t^6.88/(g1^2*y) - (g1*t^7.06)/y + t^7.19/(g1*y) + (g1^2*t^7.37)/y + t^7.5/y + t^7.63/(g1^2*y) + (2*g1^3*t^7.68)/y + (g1*t^7.81)/y + (3*t^7.94)/(g1*y) + (3*g1^2*t^8.12)/y + t^8.25/y + (2*t^8.38)/(g1^2*y) + (2*g1^3*t^8.43)/y + (4*g1*t^8.56)/y + (2*t^8.69)/(g1*y) - (g1^4*t^8.75)/y + (6*g1^2*t^8.87)/y - t^4.5*y - g1^2*t^6.62*y - (t^6.88*y)/g1^2 - g1*t^7.06*y + (t^7.19*y)/g1 + g1^2*t^7.37*y + t^7.5*y + (t^7.63*y)/g1^2 + 2*g1^3*t^7.68*y + g1*t^7.81*y + (3*t^7.94*y)/g1 + 3*g1^2*t^8.12*y + t^8.25*y + (2*t^8.38*y)/g1^2 + 2*g1^3*t^8.43*y + 4*g1*t^8.56*y + (2*t^8.69*y)/g1 - g1^4*t^8.75*y + 6*g1^2*t^8.87*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
47245 SU2adj1nf2 $\phi_1q_1^2$ + $ \phi_1^4$ + $ M_1q_2\tilde{q}_2$ + $ M_2\phi_1q_2\tilde{q}_1$ + $ M_2q_1\tilde{q}_2$ + $ M_3\phi_1\tilde{q}_1^2$ + $ M_2M_4$ + $ M_5\phi_1q_2^2$ 0.6463 0.8266 0.7818 [X:[], M:[1.1141, 0.75, 0.7718, 1.25, 0.7282], q:[0.75, 0.3859], qb:[0.3641, 0.5], phi:[0.5]] t^2.18 + t^2.25 + t^2.32 + t^2.59 + t^3. + 2*t^3.34 + t^3.41 + 2*t^3.75 + t^4.09 + t^4.16 + t^4.37 + t^4.43 + 3*t^4.5 + t^4.57 + t^4.63 + t^4.78 + t^4.84 + t^4.91 + 2*t^5.18 + t^5.25 + t^5.32 + 2*t^5.53 + 3*t^5.59 + 2*t^5.66 + t^5.72 + 3*t^5.93 - t^4.5/y - t^4.5*y detail