/*
Author : Chandan Agrawal
College : Poornima College of Engg. jaipur, Raj
Mail : chandanagrawal23@gmail.com
" when you are not practicing someone else is ,
and the day u meet them u will lose "
*/
#include<bits/stdc++.h>
#include<stdio.h>
using namespace std;
#define fastio ios_base::sync_with_stdio(false);cin.tie(0);cout.tie(0);
#define MAX 200050
#define ll long long
#define ld long double
#define lli long long int
#define pb push_back
#define INF 1000000000000
#define mod 1000000007
// trignometric function always give value in Radians only
#define PI acos(-1) //3.1415926535897932384626433832795028
#define dsin(degree) sin(degree*(PI/180.0))
#define dcos(degree) cos(degree*(PI/180.0))
#define dtan(degree) tan(degree*(PI/180.0))
#define rsin(radian) sin(radian)
#define rcos(radian) cos(radian)
#define rtan(radian) tan(radian)
#define mem0(a) memset(a,0,sizeof(a))
#define mem1(a) memset(a,-1,sizeof(a))
#define memf(a) memset(a,false,sizeof(a))
#define loop(i,n) for (lli i = 0; i < n; i++)
#define FOR(i,a,b) for (lli i = a; i < b; i++)
#define all(v) v.begin(),v.end()
#define rall(v) v.rbegin(),v.rend()
#define sz(x) int(x.size())
#define F first
#define S second
#define mii map<lli,lli>
#define pii pair<lli,lli>
#define vi vector<lli>
#define vvi vector<vi>
#define vpi vector<pii>
#define vbool vector<bool>
#define seti set<lli>
#define gcd(a,b) __gcd((a),(b))
#define lcm(a,b) (a/gcd(a,b))*b
#define abs(x) ((x < 0)?-(x):x)
#define endl '\n'
template <typename T>
void print(T x){cout<<x<<endl;}
template <typename T1, typename T2>
void print2(T1 x,T2 y){cout<<x<<" "<<y<<endl;}
template <typename T1, typename T2,typename T3>
void print3(T1 x, T2 y,T3 z){cout<<x<<" "<<y<<" "<<z<<endl;}
#define scanarr(a,n) for(lli i=0;i<n;i++) cin>>a[i];
#define scanvec(a,n) for(lli i=0;i<n;i++){ lli x ; cin>>x; a.pb(x);}
#define printarr(a,n) for(lli i=0;i<n;i++) cout<<a[i]<<" "; cout<<endl;
#define printvec(vec) for(auto xt : vec) cout<<xt<<" "; cout<<"\n";
#define FD(N) fixed<<setprecision(N)
#define deb(x) cout<<#x<<" "<<x<<endl;
/*
1D vector - vi dp(n,value);
2D vector - vvi dp(n,vi(n,value));
*/
// chandan1,2
void chandan1(){int y=1;return;}
void chandan2(){
loop(i,10){
lli x=1;
}
return(chandan1());
}
vi adj[MAX];
// minimum length cycle in graph -
lli bfs(lli src , lli n)
{
lli res = INF;
vi dist(n+1 , INF);
vi parent(n+1,-1);
queue<lli>q;
q.push(src);
dist[src]=0;
while(!q.empty())
{
lli u = q.front();q.pop();
for(auto child : adj[u])
{
if(child == parent[u]) continue; // means ham node u ko hi dekh rahe hai jo ki child ka hi adjacent hai
if(dist[child] == INF ) // means they are unvisited
{
dist[child] = dist[u]+1;
q.push(child);
parent[child] = u;
}
else
{
// means there is a cycle;
//The to vertex has already been visited. Loop found. There is a path from start to u of length d [ u ] and from start to to of length d [ to ].
//At the moment we have met an edge ( u , to ) forming a cycle. The cycle length is d [ to ] + d [ u ] + 1
res = min(res , (dist[u] + dist[child] +1 ));
if(res == 3)
return 3; //If the length of the cycle has become equal to 3, then it can no longer decrease.
}
}
}
return res;
}
int main(){
fastio
lli t=1;
cin>>t;
chandan2();
loop(qw,t) {
cout<<"Case "<<qw+1<<": ";
lli n,m;
cin>>n>>m;
loop(i,m)
{
lli x,y;
cin>>x>>y;
adj[x+1].pb(y+1);
adj[y+1].pb(x+1);
}
lli ans = INF;
FOR(i,1,n+1)
{
ans = min(ans , bfs(i,n));
if(ans == 3)
break;
}
if(ans == INF)
print("impossible");
else
print(ans);
FOR(i,1,n+1)
adj[i].clear();
}
return 0;
}
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