Landscape

Select a theory SU(2): 4 fund + 4 anti-fund (not completed) SU(2): 1 Adj + 1 fund + 1 anti-fund SU(2): 1 Adj + 2 fund + 2 anti-fund (not completed) SU(2): 1 Adj + 3 fund + 3 anti-fund (not completed) SU(3): 1 Adj + 1 fund + 1 anti-fund SU(3): 1 Adj + 2 fund + 2 anti-fund (not completed) SO(5): 5 vector (not completed) SO(5): 1 Adj + 1 vector SO(5): 1 Adj + 2 vector SO(5): 1 Symm SO(5): 1 Symm + 1 vector SO(5): 1 Symm + 2 vector Sp(2): 1 Adj + 2 fund Sp(2): 1 14 + 2 fund Sp(2): 2 Adj G2: 1 Adj + 1 fund All theories

$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =

Check if you want only theories with rational charges.

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.

#	Theory	Superpotential	Central charge $a$	Central charge $c$	Ratio $a/c$	Matter field: $R$-charge	U(1) part of $F_{UV}$	Rank of $F_{UV}$	Rational
3993	SU2adj1nf2	$\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_1M_5$ + $ M_6\phi_1\tilde{q}_1^2$ + $ M_1M_7$ + $ M_3M_8$	0.6307	0.7848	0.8036	[X:[], M:[1.2095, 1.1937, 0.8221, 0.7905, 0.7905, 0.7748, 0.7905, 1.1779], q:[0.7984, 0.3795], qb:[0.411, 0.7984], phi:[0.4032]]	[X:[], M:[[-6], [4], [-14], [6], [6], [16], [6], [14]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]]	1

Relevant Operators	Marginal Operators	$n_{marginal}$$-$$|F_{IR}|$	Superconformal Index	Refined index
$M_6$, $ M_4$, $ M_5$, $ M_7$, $ \phi_1q_2^2$, $ M_8$, $ q_1q_2$, $ M_2$, $ \phi_1q_2\tilde{q}_1$, $ M_6^2$, $ M_4M_6$, $ M_5M_6$, $ M_6M_7$, $ M_4^2$, $ M_4M_5$, $ M_5^2$, $ M_4M_7$, $ M_5M_7$, $ M_7^2$, $ \phi_1q_2\tilde{q}_2$, $ q_1\tilde{q}_2$, $ M_6\phi_1q_2^2$, $ M_6M_8$, $ M_6q_1q_2$, $ M_4\phi_1q_2^2$, $ M_5\phi_1q_2^2$, $ M_7\phi_1q_2^2$, $ M_2M_6$, $ M_4M_8$, $ M_5M_8$, $ M_7M_8$, $ M_4q_1q_2$, $ M_5q_1q_2$, $ M_7q_1q_2$, $ M_6\phi_1q_2\tilde{q}_1$, $ M_2M_4$, $ M_2M_5$, $ M_2M_7$, $ M_4\phi_1q_2\tilde{q}_1$, $ M_5\phi_1q_2\tilde{q}_1$, $ M_7\phi_1q_2\tilde{q}_1$	$\phi_1\tilde{q}_2^2$	-3	t^2.32 + 3*t^2.37 + t^3.49 + 2*t^3.53 + 2*t^3.58 + t^4.65 + 3*t^4.7 + 6*t^4.74 + t^4.79 + t^5.81 + 5*t^5.86 + 7*t^5.91 + 4*t^5.95 - 3*t^6. - 2*t^6.05 - t^6.09 + 2*t^6.97 + 5*t^7.02 + 10*t^7.07 + 12*t^7.11 + t^7.16 - 4*t^7.21 - 3*t^7.26 - t^7.3 + t^8.14 + 5*t^8.18 + 13*t^8.23 + 13*t^8.28 + 3*t^8.32 - 11*t^8.37 - 8*t^8.42 - 4*t^8.47 - t^4.21/y - t^6.53/y - (2*t^6.58)/y + (3*t^7.7)/y + (3*t^7.74)/y + (2*t^7.84)/y + t^7.89/y + t^8.81/y + (4*t^8.86)/y + (6*t^8.91)/y + (3*t^8.95)/y - t^4.21*y - t^6.53*y - 2*t^6.58*y + 3*t^7.7*y + 3*t^7.74*y + 2*t^7.84*y + t^7.89*y + t^8.81*y + 4*t^8.86*y + 6*t^8.91*y + 3*t^8.95*y	g1^16*t^2.32 + 3*g1^6*t^2.37 + g1^24*t^3.49 + 2*g1^14*t^3.53 + 2*g1^4*t^3.58 + g1^32*t^4.65 + 3*g1^22*t^4.7 + 6*g1^12*t^4.74 + g1^2*t^4.79 + g1^40*t^5.81 + 5*g1^30*t^5.86 + 7*g1^20*t^5.91 + 4*g1^10*t^5.95 - 3*t^6. - (2*t^6.05)/g1^10 - t^6.09/g1^20 + 2*g1^48*t^6.97 + 5*g1^38*t^7.02 + 10*g1^28*t^7.07 + 12*g1^18*t^7.11 + g1^8*t^7.16 - (4*t^7.21)/g1^2 - (3*t^7.26)/g1^12 - t^7.3/g1^22 + g1^56*t^8.14 + 5*g1^46*t^8.18 + 13*g1^36*t^8.23 + 13*g1^26*t^8.28 + 3*g1^16*t^8.32 - 11*g1^6*t^8.37 - (8*t^8.42)/g1^4 - (4*t^8.47)/g1^14 - t^4.21/(g1^2*y) - (g1^14*t^6.53)/y - (2*g1^4*t^6.58)/y + (3*g1^22*t^7.7)/y + (3*g1^12*t^7.74)/y + (2*t^7.84)/(g1^8*y) + t^7.89/(g1^18*y) + (g1^40*t^8.81)/y + (4*g1^30*t^8.86)/y + (6*g1^20*t^8.91)/y + (3*g1^10*t^8.95)/y - (t^4.21*y)/g1^2 - g1^14*t^6.53*y - 2*g1^4*t^6.58*y + 3*g1^22*t^7.7*y + 3*g1^12*t^7.74*y + (2*t^7.84*y)/g1^8 + (t^7.89*y)/g1^18 + g1^40*t^8.81*y + 4*g1^30*t^8.86*y + 6*g1^20*t^8.91*y + 3*g1^10*t^8.95*y

Deformation

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

#	Superpotential	Central Charge $a$	Central Charge $c$	Ratio $a/c$	$R$-charges	Superconformal Index	More Info.	Rational

Equivalent Fixed Points from Other Seed Theories

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

#	Theory	Superpotential	Central Charge $a$	Central Charge $c$	Ratio $a/c$	$R$-charges	Superconformal Index	More 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.

#	Theory	Superpotential	Central Charge $a$	Central Charge $c$	Ratio $a/c$	$R$-charges	Superconformal Index	More Info.	Rational
1609	SU2adj1nf2	$\phi_1q_1^2$ + $ M_1q_2\tilde{q}_1$ + $ M_2\phi_1^2$ + $ M_3q_2\tilde{q}_2$ + $ M_4\tilde{q}_1\tilde{q}_2$ + $ M_1M_4$ + $ M_5q_1\tilde{q}_1$ + $ M_1M_5$ + $ M_6\phi_1\tilde{q}_1^2$ + $ M_1M_7$	0.6465	0.8092	0.799	[X:[], M:[1.2006, 1.1996, 0.8013, 0.7994, 0.7994, 0.7985, 0.7994], q:[0.7999, 0.3988], qb:[0.4007, 0.7999], phi:[0.4002]]	5*t^2.4 + t^3.59 + 3*t^3.6 + 4*t^4.79 + 11*t^4.8 + t^4.81 + 9*t^5.99 + 3*t^6. - t^4.2/y - t^4.2*y	detail